diff --git a/.gitignore b/.gitignore index 8c260d6e70..551e709ddf 100644 --- a/.gitignore +++ b/.gitignore @@ -66,7 +66,5 @@ target/ .idea/ # Locally generated certificates for development -elasticsearch-proxy/nginx.crt -elasticsearch-proxy/nginx.key nginx/localhost.crt nginx/localhost.key diff --git a/.inveniorc b/.inveniorc index bd9f869cf7..46e6e7ba9a 100755 --- a/.inveniorc +++ b/.inveniorc @@ -13,7 +13,6 @@ export INVENIO_POSTGRESQL_DBNAME=cernopendata export INVENIO_POSTGRESQL_DBUSER=cernopendata export INVENIO_POSTGRESQL_DBPASS=dbpass123 export INVENIO_REDIS_HOST=192.168.50.12 -export INVENIO_ELASTICSEARCH_HOST=192.168.50.13 export INVENIO_RABBITMQ_HOST=192.168.50.14 export INVENIO_WORKER_HOST=192.168.50.15 # sphinxdoc-kickstart-configuration-variables-end diff --git a/Dockerfile b/Dockerfile index 5f325987c9..e678a0f035 100644 --- a/Dockerfile +++ b/Dockerfile @@ -25,8 +25,8 @@ # Use Invenio's alma image with Python-3.9 FROM registry.cern.ch/inveniosoftware/almalinux:1 -# Use XRootD 5.6.6 -ENV XROOTD_VERSION=5.6.6 +# Use XRootD 5.6.8 +ENV XROOTD_VERSION=5.6.8 # Install CERN Open Data Portal web node pre-requisites # hadolint ignore=DL3033 diff --git a/MANIFEST.in b/MANIFEST.in index 033d2e04e0..004165b085 100644 --- a/MANIFEST.in +++ b/MANIFEST.in @@ -9,8 +9,6 @@ include .inveniorc include Dockerfile include LICENSE include babel.ini -include elasticsearch-proxy/Dockerfile -include elasticsearch-proxy/nginx.conf include nginx/Dockerfile include pytest.ini include sentry/Dockerfile @@ -45,4 +43,3 @@ recursive-include sentry *.json recursive-include sentry *.py recursive-include sentry *.sh recursive-include sentry *.yml -recursive-exclude elasticsearch-proxy * diff --git a/cernopendata/config.py b/cernopendata/config.py index ae9a27eb8b..10f4b5e542 100644 --- a/cernopendata/config.py +++ b/cernopendata/config.py @@ -56,7 +56,7 @@ # Piwik tracking code: set None to disabled it THEME_PIWIK_ID = os.environ.get("PIWIK_ID", None) - +ACCOUNTS_SESSION_ACTIVITY_ENABLED = None SITE_URL = os.environ.get("CERNOPENDATA_SITE_URL", "opendata.cern.ch") # Logging - Set up Sentry for Invenio-Logging @@ -91,6 +91,17 @@ "data:", "https://cdnjs.cloudflare.com", ], + "img-src": [ + "'self'", + "cms-results.web.cern.ch", + "raw.githubusercontent.com", + "www.github.com", + "github.com", + "cms-docdb.cern.ch", + "mybinder.org", + "cms-results.web.cern.ch", + "cds.cern.ch", + ], }, "content_security_policy_report_uri": None, "content_security_policy_report_only": False, @@ -427,10 +438,8 @@ def _query_parser_and(qstr=None): CERNOPENDATA_DISABLE_DOWNLOADS = os.environ.get("CERNOPENDATA_DISABLE_DOWNLOADS", False) # Search # ====== -#: Default Elasticsearch document type. +#: Default OpenSearch document type. SEARCH_DOC_TYPE_DEFAULT = None -#: Do not map any keywords. -SEARCH_ELASTIC_KEYWORD_MAPPING = {} # This one can be used to have multiple instances on the same cluster # SEARCH_INDEX_PREFIX = "opendata-dev-" @@ -447,7 +456,7 @@ def _query_parser_and(qstr=None): SEARCH_UI_SEARCH_VIEW = search_legacy # OAI-PMH # ======= -#: Default Elasticsearch index. +#: Default OpenSearch index. OAISERVER_RECORD_INDEX = "records" #: OAI ID prefix. OAISERVER_ID_PREFIX = "oai:opendata.cern.ch:recid/" diff --git a/cernopendata/jsonschemas/records/record-v1.0.0.json b/cernopendata/jsonschemas/records/record-v1.0.0.json index 8076c1ca66..539919e42d 100644 --- a/cernopendata/jsonschemas/records/record-v1.0.0.json +++ b/cernopendata/jsonschemas/records/record-v1.0.0.json @@ -165,6 +165,44 @@ }, "type": "object" }, + "cross_section": { + "properties": { + "filter_efficiency": { + "description": "Cross section filter efficiency as given by GenXSecAnalyser", + "type": "string" + }, + "matching_efficiency": { + "description": "Cross section matching efficiency as given by GenXSecAnalyser", + "type": "string" + }, + "neg_weight_fraction": { + "description": "Cross section negative weight fraction as given by GenXSecAnalyser", + "type": "string" + }, + "total_value": { + "description": "Cross section total value as given by GenXSecAnalyser (in pb)", + "type": "string" + }, + "total_value_uncertainty": { + "description": "Cross section total uncertainty as given by GenXSecAnalyser (in pb)", + "type": "string" + } + }, + "type": "object" + }, + "dataset_semantics_files": { + "properties": { + "url": { + "description": "Url of the dataset content description html file", + "type": "string" + }, + "json": { + "description": "Name of the dataset content description json file", + "type": "string" + } + }, + "type": "object" + }, "dataset_semantics": { "items": { "properties": { diff --git a/cernopendata/mappings/os-v2/__init__.py b/cernopendata/mappings/os-v2/__init__.py index ed3ee80aaa..11a032d50f 100644 --- a/cernopendata/mappings/os-v2/__init__.py +++ b/cernopendata/mappings/os-v2/__init__.py @@ -22,4 +22,4 @@ # waive the privileges and immunities granted to it by virtue of its status # as an Intergovernmental Organization or submit itself to any jurisdiction. -"""CERN Open Data Elasticsearch v7 Mappings.""" +"""CERN Open Data OpenSearch v7 Mappings.""" diff --git a/cernopendata/modules/fixtures/data/docs/cms-about/cms-about.md b/cernopendata/modules/fixtures/data/docs/cms-about/cms-about.md index ff4ddddb56..2bd2cdbe2b 100644 --- a/cernopendata/modules/fixtures/data/docs/cms-about/cms-about.md +++ b/cernopendata/modules/fixtures/data/docs/cms-about/cms-about.md @@ -3,7 +3,7 @@ The Compact Muon Solenoid (CMS) is one of the large particle detectors at CERN's You can find usage instructions and suggestions of CMS Open Data for different scopes in: * [Guide page to education use of CMS Open Data](/docs/cms-guide-for-education) -* In a separate [CMS Open Data guide](https://cms-opendata-guide.web.cern.ch/) (under construction). +* In a separate [CMS Open Data guide](https://cms-opendata-guide.web.cern.ch/). This page gives a brief overview of CMS Open Data contents: @@ -23,35 +23,79 @@ The following are provided through this portal: * Examples of [simplified datasets](/search?page=1&size=20&subtype=Derived&type=Dataset&experiment=CMS) derived from the primary ones for use in different applications and analyses * Tools * Downloadable [container images](/docs/cms-guide-docker) with the CMS software environment through which the datasets can be accessed - * Alternatively, a downloadable [Virtual Machine (VM)](/docs/cms-virtual-machine-2015) image with the CMS software environment - * [Getting started instructions](/docs/cms-getting-started-2015) for reading the primary dataset and producing intermediate derived data for the final analysis + * Alternatively, a downloadable [Virtual Machine (VM)](https://opendata.cern.ch/search?page=1&size=20&tags=VM&experiment=CMS) image with the CMS software environment + * Getting started instructions for reading and processing primary data in the [AOD format (Run 1)](/docs/cms-getting-started-aod), [MiniAOD format (Run 2)](/docs/cms-getting-started-miniaod), or [NanoAOD format (Run 2)](/docs/cms-getting-started-nanoaod). * Ready-to-use online applications, such as [an event display](/visualise/events/cms) and [simple histogramming software](/visualise/histograms/cms) * Source code for the various examples and applications, available in the [CMS software](/search?page=1&size=20&q=&type=Software&experiment=CMS) collection * Guides - * Set of [topical guide pages](http://opendata.cern.ch/search?page=1&size=20&q=&subtype=Guide&type=Documentation&experiment=CMS), a comprehensive set of instructions is being collected in a separate [CMS Open Data guide](https://cms-opendata-guide.web.cern.ch/) with links to the latest tutorials. + * Set of [topical guide pages](http://opendata.cern.ch/search?page=1&size=20&q=&subtype=Guide&type=Documentation&experiment=CMS) + * A omprehensive set of instructions is being collected in a separate [CMS Open Data guide](https://cms-opendata-guide.web.cern.ch/) with links to the latest tutorials. ## Primary and simulated datasets -* Collision data in the primary datasets are in a format known as AOD or Analysis Object Data, while simulated data are in a format called AODSIM. -* AOD/AODSIM files contain the information that is needed for analysis: - * all the high-level [physics objects](/docs/cms-physics-objects-2015) (such as muons, electrons, etc.); - * tracks with associated hits, calorimetric clusters with associated hits, vertices; and - * information about event selection (triggers), data needed for further selection and identification criteria for the physics objects. -* The file is not the final event interpretation with a simple list of particles. - * It contains several instances of the same physics object (i.e. a jet reconstructed with different algorithms). - * It may have double-counting (i.e. a physics object may appear as a single object of its own type, but it may also be part of a jet). - * Additional knowledge is needed to define a "good" physics object. - * Definition of same objects is different in each analysis. -* Some datasets, such as those containing heavy-ion data, are provided in a format called RECO, which contains more information than the AOD format. This is done when the original analyses by the CMS collaboration were performed using this particular format. -* Starting from Run2 (2015), datasets are provided in the MiniAOD/MiniAODSIM format, which has superseded the AOD format in physics analysis: - * MiniAOD/MiniAODSIM is approximately one tenth of the size of AOD/AODSIM. - * The reduction is obtained defining light-weight physics-object candidate representations, increasing transverse momentum thresholds for storing physics-object candidates, and reduced numerical precision when it is not required at the analysis level. - * More information on the MiniAOD format - * [Mini-AOD: A New Analysis Data Format for CMS](https://doi.org/10.1088/1742-6596/664/7/072052) - * [MiniAOD analysis documentation](https://twiki.cern.ch/twiki/bin/view/CMSPublic/WorkBookMiniAOD2015) -* The files can be read in [ROOT](http://root.cern.ch/), but they cannot be opened (and understood) as simple data tables. -* Only the runs that are validated by data quality monitoring should be used in any analysis. The [list of the validated runs](/search?page=1&size=20&q=&type=Environment&subtype=Validation) is provided. -* Small samples of [raw data](/search?page=1&size=20&q=&experiment=CMS&file_type=raw) are also provided. +Collision data in the primary datasets are typically in a format known as AOD or Analysis Object Data, while simulated data are in a format called AODSIM. Beginning in Run 2, smaller +data formats called MiniAOD and NanoAOD were developed in CMS to implement common physics object processing and remove information that not often needed for analysis. + +**AOD(SIM) and MiniAOD(SIM) files** + +AOD/AODSIM files are provided for Run 1 primary datasets and contain the information that is needed for analysis: + +* all the high-level [physics objects](/docs/cms-physics-objects-2015) (such as muons, electrons, etc.); +* tracks with associated hits, calorimetric clusters with associated hits, vertices; +* candidate particles created by the Particle Flow algorithm; +* information about event selection (triggers), data needed for further selection and identification criteria for the physics objects. + +See the [Getting Started page for AOD data](/docs/cms-getting-started-aod) to learn more about analyzing AOD files. + +Starting from Run 2 (2015), MiniAOD/MiniAODSIM files are provided. These files contain similar information to AOD, but physics objects are processed to include more +identification and selection information within a lighter C++ object, transverse momentum thresholds for storing objects are increased, +and some lower-level information has been removed. +MiniAOD datasets are appoximately one tenth of the size of AOD datasets. More information about MiniAOD: + +* [Mini-AOD: A New Analysis Data Format for CMS](https://doi.org/10.1088/1742-6596/664/7/072052) +* [MiniAOD analysis documentation](https://twiki.cern.ch/twiki/bin/view/CMSPublic/WorkBookMiniAOD2015) +* [Getting Started with CMS MiniAOD data](/docs/cms-getting-started-miniaod) + +AOD and MiniAOD files do not contain the final event interpretation with a simple list of particles. +The files can be read in [ROOT](http://root.cern.ch/), but they cannot be opened (and understood) as simple data tables. +A file typically contains several instances of the same physics object +(i.e. a jet reconstructed with different algorithms), and some physics objects may be "double-counted" (i.e. a physics object may appear as a single object of its own type, but +it may also be part of a jet). + +Additional knowledge is needed to define a "good" physics object, and this definition can be different in each analysis. +Only the runs that are validated by data quality monitoring should be used in any analysis. +The [list of the validated runs](/search?page=1&size=20&q=&type=Environment&subtype=Validation) is provided. + +**NanoAOD(SIM) files** + +Starting from data collected in 2016, datasets in NanoAOD format are provided alongside MiniAOD. +Only a limited set of observables for each physics object is kept, with limited numerical precision. +For example, detector information is typically dropped in favor of pre-computed identification algorithm results. +The Particle Flow candidates are also dropped, since they are primarily used as inputs to higher-level physics object +reconstruction. The NanoAOD format is about 20 times smaller than MiniAOD, or about 200 times smaller than AOD. +NanoAOD files can be read in [ROOT](http://root.cern.ch) as a basic `TTree` containing standard data types. +More information about NanoAOD: + +* [The NanoAOD event data format in CMS](https://doi.org/10.1088/1742-6596/1525/1/012038) +* [NanoAOD file documentation](https://twiki.cern.ch/twiki/bin/view/CMSPublic/WorkBookNanoAOD) +* [Getting Started with CMS NanoAOD data](/docs/cms-getting-started-nanoaod) + +NanoAOD files may still contain several instances of the same physics object +(i.e. a jet reconstructed with different algorithms), and some physics objects may be "double-counted" (i.e. a physics object may appear as a single object of its own type, but +it may also be part of a jet). + +Additional knowledge is needed to define a "good" physics object, and this definition can be different in each analysis. +Only the runs that are validated by data quality monitoring should be used in any analysis. +The [list of the validated runs](/search?page=1&size=20&q=&type=Environment&subtype=Validation) is provided. + +**RECO files** + +Some datasets, such as those containing heavy-ion data, are provided in a format called RECO, which contains more information than the AOD format. +This is done when the original analyses by the CMS collaboration were performed using this particular format. + +**Raw data** + +Small samples of [raw data](/search?page=1&size=20&q=&experiment=CMS&file_type=raw) are also provided. ## Disclaimer @@ -67,6 +111,7 @@ The following are provided through this portal: * The release of 2012 data includes a larger sample of simulated data. A part of 2012 simulated data is released with the bibliographic information content only, and these datasets will be made available online on demand. * The release of 2013 heavy-ion-related data includes simulated data corresponding to different collision types and centre-of mass energies. * The release of 2015 data includes a large collection of simulated data, reprocessed with a software release compatible with the 2015 collision data, but it may still happen that some simulated data did not make it to this reprocessing and are therefore not available in this collection. + * The release of 2016 data includes a large collection of simulated data, reprocessed with a software release compatible with the 2016 collision data. * If you are interested in joining the CMS Collaboration, please read [How to join CMS](https://cms.cern/collaboration/how-join-cms). ## Other CMS open data @@ -77,4 +122,4 @@ The following are provided through this portal: ## Policies * [Data preservation and open access policy](/record/415) -* [Papers by CMS members using public data [internal]](https://cms-docdb.cern.ch/cgi-bin/DocDB/ShowDocument?docid=14372) +* [Papers by CMS members using public data [internal]](https://cms-docdb.cern.ch/cgi-bin/DocDB/ShowDocument?docid=14372) \ No newline at end of file diff --git a/cernopendata/modules/fixtures/data/docs/cms-getting-started-miniaod/cms-getting-started-miniaod.md b/cernopendata/modules/fixtures/data/docs/cms-getting-started-miniaod/cms-getting-started-miniaod.md index a6da85ed0b..87ac09e254 100644 --- a/cernopendata/modules/fixtures/data/docs/cms-getting-started-miniaod/cms-getting-started-miniaod.md +++ b/cernopendata/modules/fixtures/data/docs/cms-getting-started-miniaod/cms-getting-started-miniaod.md @@ -36,7 +36,7 @@ $ cmsenv # do not execute this command if you are working in the container
2016

-To analyse CMS data collected in 2016, you need version 10.6.30 of CMSSW, supported on Scientific Linux 7. Once you have installed the CMS open data container or the CMS-specific CERN Virtual Machine (VM), you need to open a terminal. +To analyse CMS data collected in 2016, you need version 10.6.30 of CMSSW, supported on Scientific Linux 7. Once you have installed the CMS open data container or the CMS-specific CERN Virtual Machine (VM), you need to open a terminal.

If you are using the VM, always use the "CMS shell" terminal available from the "CMS Shell" icon on the desktop for all CMSSW-specific commands, such as compilation and run. In the VM, execute the following command in the terminal if you haven't done so before; it ensures that you have this version of CMSSW running: diff --git a/cernopendata/modules/fixtures/data/docs/cms-guide-docker/cms-guide-docker.md b/cernopendata/modules/fixtures/data/docs/cms-guide-docker/cms-guide-docker.md index 54466c9bb5..cd240ec76d 100644 --- a/cernopendata/modules/fixtures/data/docs/cms-guide-docker/cms-guide-docker.md +++ b/cernopendata/modules/fixtures/data/docs/cms-guide-docker/cms-guide-docker.md @@ -1,15 +1,18 @@ 1. [Introduction](#intro) +2. [Available general-purpose container images](#nanoaod) 2. [Available CMSSW container images](#images) -3. [Fetch a CMSSW image and start a container](#fetch-start) +3. [Fetch an image and start a container](#fetch-start) 4. [Useful commands](#commands) 1. [Exiting and restarting a container](#exit-start) - 2. [Copying files](#cp) - 3. [Execute a command in a running container](#exec) - 4. [Removing a container](#rm) + 2. [Removing a container](#rm) + 3. [Copying files](#cp) + 4. [Mounting a local file area](#mount) + 5. [Execute a command in a running container](#exec) 5. [Graphics](#graphics) 1. [VNC](#vnc) 2. [X11 forwarding on Linux](#x11) 3. [Test graphics](#test-graphics) + 4. [Launching Jupyter in the Python container](#jupyter) 6. [Container prompt](#prompt) 7. [Install and run CMS example code](#get-started) 8. [Running CMS open data containers on WSL2](#on-wsl2) @@ -19,11 +22,44 @@ You can run CMS analysis code in a [Docker](https://www.docker.com/) container provided together with the CMS open data. If you have not already installed Docker, instructions for installation are [provided by Docker](https://docs.docker.com/install/). For an introduction and for getting started, you can follow the links provided in [the CMS Open data guide](https://cms-opendata-guide.web.cern.ch/tools/docker/). +## Available general-purpose container images + +The quickest way to get started analyzing CMS open data is to consider data in the NanoAOD format, either [derived data from +Run 1](https://opendata.cern.ch/search?q=&f=experiment%3ACMS&f=type%3ADataset%2Bsubtype%3ADerived&l=list&order=desc&p=1&s=10&sort=mostrecent) or [NanoAOD from Run 2](https://opendata.cern.ch/search?q=&f=experiment%3ACMS&f=file_type%3Ananoaod&f=file_type%3Ananoaodsim). These file formats can be analyzed using ROOT and python tools. The container images linked +here contain the packages required to access open data files over the network. + +**ROOT container**: this image contains ROOT 6 coupled with Python 3 and a VNC server for access to the graphical user interface. + +**Python container**: this images contains Python 3 with a HEP software stack and a VNC server for access to the graphical user interface. HEP-related python packages in this image include `awkward`, `uproot`, `numpy`, `matplotlib`, and `jupyterlab`. + + + + + + + + + + + + + + + + + + + + + +
Software
Container image (dockerhub)Alternative image location (GitLab)
ROOTcmscloud/root-vncgitlab-registry.cern.ch/cms-cloud/root-vnc:latest
Pythoncmscloud/python-vncgitlab-registry.cern.ch/cms-cloud/python-vnc:latest
+ + ## Available CMSSW container images For the first access of each set of CMS open data, you will need a specific container image containing the software corresponding to that particular set of data. The following images are available: - +
@@ -130,14 +166,15 @@ gitlab-registry.cern.ch/cms-cloud/cmssw-docker-opendata/cmssw_3_9_2_patch5-slc5_
-## Fetch a CMSSW image and start a container +## Fetch an image and start a container -In the following instructions, make sure to replace the CMSSW version and the container image name according to the table above. These commands are for 2015 proton-proton data, with the CMSSW version 7_6_7 and the `cmssw_7_6_7-slc6_amd64_gcc493` container image. +In the following instructions, make sure to replace the example container image name according to the table above. +These commands are for 2015 proton-proton data, with the CMSSW version 7_6_7 and the `cmssw_7_6_7-slc6_amd64_gcc493` container image. -Once you have installed Docker on your computer, you can fetch a CMSSW image, and create and start a container using the `docker run` command: +Once you have installed Docker on your computer, you can fetch a container image, and create and start a container using the `docker run` command: ```sh -docker run --name my_od -P -p 5901:5901 -p 6080:6080 -it cmsopendata/cmssw_7_6_7-slc6_amd64_gcc493 /bin/bash +docker run -it --name my_od -P -p 5901:5901 -p 6080:6080 cmsopendata/cmssw_7_6_7-slc6_amd64_gcc493 /bin/bash ``` Here we fetch the `cmssw_7_6_7-slc6_amd64_gcc493` docker image from [dockerhub](https://hub.docker.com/u/cmsopendata) and name the container `my_od`. @@ -145,7 +182,7 @@ Here we fetch the `cmssw_7_6_7-slc6_amd64_gcc493` docker image from [dockerhub]( This will install a stand-alone CMSSW image (several gigabytes). Therefore this may take a while. However, the image will only have to be downloaded once. The following will appear in your terminal, with messages changing during the download: ```console -$ docker run --name my_od -P -p 5901:5901 -p 6080:6080 -it cmsopendata/cmssw_7_6_7-slc6_amd64_gcc493 /bin/bash +$ docker run -it --name my_od -P -p 5901:5901 -p 6080:6080 cmsopendata/cmssw_7_6_7-slc6_amd64_gcc493 /bin/bash Unable to find image 'cmsopendata/cmssw_7_6_7-slc6_amd64_gcc493:latest' locally latest: Pulling from cmsopendata/cmssw_7_6_7-slc6_amd64_gcc493 a34e8f61dde2: Already exists @@ -179,7 +216,7 @@ CMSSW should now be available. This is a standalone image for CMSSW_7_6_7 slc6_amd64_gcc493. ``` -Once done, you should see the commmand prompt for the CMSSW instance within Docker: +Once done, in a CMSSW container you should see the commmand prompt for the CMSSW instance within Docker: ```console (/code/CMSSW_7_6_7/src) @@ -187,11 +224,18 @@ Once done, you should see the commmand prompt for the CMSSW instance within Dock If you are using a linux distribution on WSL2, and do not get this prompt, but get back to your local terminal prompt, see the instructions [below](#on-wsl2) under "Running CMS open data containers on WSL2". +**Non-CMSSW containers**: in the ROOT or Python containers the pull output will look very similar to the example above, +but without any messages about setting up CMSSW. After the image has been downloaded you will see a command prompt in the `code/` directory: + +```console +(/code) +``` + ## Useful commands In the following, some useful commands are given. For a complete list of commands, see the [docker command line documentation](https://docs.docker.com/engine/reference/commandline/cli/). -### Exiting and restarting a container +#### Exiting and restarting a container When you want to exit the container simply type `exit`. @@ -201,50 +245,69 @@ If you want to restart the container (e.g. the one named `my_od`) and return to docker start -i my_od ``` -### Copying files +#### Removing a container + +You can remove the container `my_od` with + +```sh +docker rm my_od +``` + +This does not remove the image, which took long to download. You can create a new container from that image with the same `docker run ...` command as above, but it will be much faster than the first time. + +If the container was created and started using the `--rm` option (e.g. `docker run --rm ...`) then the container will be removed when you exit. + +#### Copying files You can copy file out of a runnning container to your local computer. Create an file in the container (for example) with ```sh -echo $CMSSW_VERSION > $HOME/example.txt +echo $SHELL > $HOME/example.txt ``` -In order to copy this file out of a running container, open another terminal of your local computer and run the following command: +In order to copy this file out of a running container, open another terminal of your local computer and run one of the following commands: ```sh -docker cp my_od:/home/cmsusr/example.txt . +docker cp my_od:/home/cmsusr/example.txt . # for CMSSW container +docker cp my_od:/code/example.txt . # ROOT or Python container ``` Likewise, in order to copy a file into a running container: - ```sh -docker cp my_od:/home/cmsusr/ +docker cp my_od:/home/cmsusr/ # for CMSSW container +docker cp my_od:/code # for ROOT or Python container ``` -### Execute a command in a running container +#### Mounting a local file area in the container -You may need to submit a command from your local host into a running container. For example, to see the running processes in the `my_od` container, run: +It is possible to create a local directory system and mount it in the container, so that files are shared automatically without +needing to copy in and out of the container. If you already have a container, exit from the container and remove it using the docker rm command. For CMSSW containers in particular it is important to create the working area with the +proper permissions before creating the container. ```sh -docker exec my_od ps -ef +export workpath=$PWD +mkdir cms_open_data_work +chmod -R 777 cms_open_data_work ``` -### Removing a container - -You can remove the container `my_od` with +Then create a container that includes mounting information through the `-v` option. ```sh -docker rm my_od +docker run -it --name my_od -P -p 5901:5901 -p 6080:6080 -v ${workpath}/cms_open_data_work:/code cmsopendata/cmssw_7_6_7-slc6_amd64_gcc493 /bin/bash ``` -This does not remove the image, which took long to download. You can create a new container from that image with the same `docker run ...` command as above, but it will be much faster than the first time. +#### Execute a command in a running container -If the container was created and started using the `--rm` option (e.g. `docker run --rm ...`) then the container will be removed when you exit. +You may need to submit a command from your local host into a running container. For example, to see the running processes in the `my_od` container, run: + +```sh +docker exec my_od ps -ef +``` ## Graphics -### VNC +#### VNC For opening graphics windows, the container image has a VNC application installed. Start the VNC application in the container with @@ -264,14 +327,15 @@ stop_vnc You can find more details on the configuration and usage of VNC in the CMS open data containers in [the image repository](https://gitlab.cern.ch/cms-cloud/cmssw-docker-opendata/-/tree/master#use-vnc). -### X11 forwarding on Linux +#### X11 forwarding on Linux If you are running on a Linux computer, you can also use X11 forwarding. If you already started a container name `my_od` and now decide to use X11 forwarding instead of VNC, exit from the container shell with `exit`, remove the existing container with `docker rm my_od`. Then start a new container with ```sh docker run -it --name my_od --net=host --env="DISPLAY" -v $HOME/.Xauthority:/home/cmsusr/.Xauthority:rw cmssw_7_6_7-slc6_amd64_gcc493 /bin/bash ``` -### Test graphics + +#### Test graphics You can test if the graphics window opens by typing in the container shell @@ -288,7 +352,7 @@ This will open the ROOT browser window. You can exit ROOT with `.q` in the `root If you are new to ROOT, have a quick look to [the Getting started page](/docs/cms-getting-started-2015), or follow the links in [the CMS open data guide](https://cms-opendata-guide.web.cern.ch/tools/root/). -## Container prompt +#### Container prompt If the container prompt causes trouble for line wrapping, increase the size of the terminal. If it does not help, you can change the prompt with @@ -298,14 +362,51 @@ export PS1="(\w) " To change it permanently, add this line to the file `/home/cmsusr/.bashrc` in the container. +#### Launching Jupyter in the Python container + +The Python container supports jupyter notebook usage though the container. To access this tool, create +a new python container with port 8888 enabled as well as the other ports in the original example: + +```sh +docker run --rm -it -P -p 5901:5901 -p 6080:6080 -p 8888:8888 gitlab-registry.cern.ch/cms-cloud/python-vnc:latest +``` + +Inside the container, launch jupyter-lab with the following command. You will see output that includes a link: + +```console +$ jupyter-lab --ip=0.0.0.0 --no-browser +[I 2024-02-15 16:14:59.384 ServerApp] jupyterlab | extension was successfully linked. +[I 2024-02-15 16:14:59.395 ServerApp] nbclassic | extension was successfully linked. +[I 2024-02-15 16:14:59.397 ServerApp] Writing Jupyter server cookie secret to /home/cmsusr/.local/share/jupyter/runtime/jupyter_cookie_secret +[I 2024-02-15 16:14:59.953 ServerApp] notebook_shim | extension was successfully linked. +[I 2024-02-15 16:14:59.990 ServerApp] notebook_shim | extension was successfully loaded. +[I 2024-02-15 16:14:59.992 LabApp] JupyterLab extension loaded from /usr/local/venv/lib/python3.10/site-packages/jupyterlab +[I 2024-02-15 16:14:59.992 LabApp] JupyterLab application directory is /usr/local/venv/share/jupyter/lab +[I 2024-02-15 16:14:59.997 ServerApp] jupyterlab | extension was successfully loaded. +[I 2024-02-15 16:15:00.010 ServerApp] nbclassic | extension was successfully loaded. +[I 2024-02-15 16:15:00.010 ServerApp] Serving notebooks from local directory: /code +[I 2024-02-15 16:15:00.010 ServerApp] Jupyter Server 1.18.1 is running at: +[I 2024-02-15 16:15:00.010 ServerApp] http://ae4189a5ed44:8888/lab?token=bf6db43d28d8073b3859885d8ffcf8693785cc0d59a146ca +[I 2024-02-15 16:15:00.010 ServerApp] or http://127.0.0.1:8888/lab?token=bf6db43d28d8073b3859885d8ffcf8693785cc0d59a146ca +[I 2024-02-15 16:15:00.010 ServerApp] Use Control-C to stop this server and shut down all kernels (twice to skip confirmation). +[C 2024-02-15 16:15:00.015 ServerApp] + + To access the server, open this file in a browser: + file:///home/cmsusr/.local/share/jupyter/runtime/jpserver-9-open.html + Or copy and paste one of these URLs: + http://ae4189a5ed44:8888/lab?token=bf6db43d28d8073b3859885d8ffcf8693785cc0d59a146ca + or http://127.0.0.1:8888/lab?token=bf6db43d28d8073b3859885d8ffcf8693785cc0d59a146ca +``` + +Paste the `http` link into your browser to access a jupyter-lab session where you can create notebooks and see your existing notebooks. ## Install and run CMS example code -If you have read the instructions above, you can now follow [the getting started instructions](/docs/cms-getting-started-2015) for the first steps with the CMS open data. +If you have read the instructions above, you can now follow the getting started instructions for CMS [AOD data (Run 1)](/docs/cms-getting-started-aod), [MiniAOD data (Run 2)](/docs/cms-getting-started-miniaod), or [NanoAOD data (Run 2)](/docs/cms-getting-started-nanoaod). ## Running CMS open data containers on WSL2 -The CMS open data containers, or any CentOS6-based containers, may fail if docker is run on WSL2. This problem is fixed by adding a new file `.wslconfig` with the following contents +The CMSSW open data containers, or any CentOS6-based containers, may fail if docker is run on WSL2. This problem is fixed by adding a new file `.wslconfig` with the following contents ```sh [wsl2] @@ -344,4 +445,4 @@ The other option is to [install](https://cvmfs.readthedocs.io/en/stable/cpt-quic ```sh docker run --privileged --name my_od -it cmsopendata/cmssw_7_6_7-slc6_amd64_gcc493 /bin/bash -``` +``` \ No newline at end of file diff --git a/cernopendata/modules/fixtures/data/docs/cms-guide-for-conddb/cms-guide-for-conddb.md b/cernopendata/modules/fixtures/data/docs/cms-guide-for-conddb/cms-guide-for-conddb.md index b51f481f27..647ba2738f 100644 --- a/cernopendata/modules/fixtures/data/docs/cms-guide-for-conddb/cms-guide-for-conddb.md +++ b/cernopendata/modules/fixtures/data/docs/cms-guide-for-conddb/cms-guide-for-conddb.md @@ -5,7 +5,11 @@ 2. [Accessing condition data from the CMS Open Data containers](#containers) 4. [Global tags](#global-tags) 1. [Proton-proton data](#proton-proton) + 1. [Run-1](#pp-run1) + 2. [Run-2](#pp-run2) 2. [Heavy-ion related data](#heavy-ion) + 1. [Run-1](#hi-run1) + 2. [Run-2](#hi-run2) ## What is the condition database? @@ -74,6 +78,8 @@ The global tags for condition data are different for different data-taking perio ### Proton-proton data +#### Run-1 + --- **For 2010 collision data**, the global tag is FT_R_42_V10A. @@ -309,6 +315,8 @@ process.GlobalTag.connect = cms.string('sqlite_file:/cvmfs/cms-opendata-conddb.c process.GlobalTag.globaltag = 'START53_V27::All' ``` +#### Run-2 + --- **For 2015 collision data**, the global tag is 76X_dataRun2_16Dec2015_v0. @@ -342,6 +350,38 @@ Note that when using the CMS open data software container, the `process.GlobalTa --- +**For 2016 collision data**, the global tag is 106X_dataRun2_v37. + +**VM and container:** + +Define the correct set of condition data by mentioning the global tag in the configuration file of the job. + +```shell +#globaltag for 2016 collision data +process.GlobalTag.connect = cms.string('sqlite_file:/cvmfs/cms-opendata-conddb.cern.ch/106X_dataRun2_v37.db') +process.GlobalTag.globaltag = '106X_dataRun2_v37' +``` + +Note that when using the CMS open data software container, the `process.GlobalTag.connect` line makes the job read the condition data from the local `/cvmfs` area in the container. If it is left out, the condition data are read from predefined condition data servers and it may take longer. + +--- + +**For 2016 simulated data**, the global tag is 106X_mcRun2_asymptotic_v17. + +**VM and container:** + +Define the correct set of condition data by mentioning the global tag in the configuration file of the job. + +```shell +#globaltag for 2016 MC +process.GlobalTag.connect = cms.string('sqlite_file:/cvmfs/cms-opendata-conddb.cern.ch/106X_mcRun2_asymptotic_v17.db') +process.GlobalTag.globaltag = '106X_mcRun2_asymptotic_v17' +``` + +Note that when using the CMS open data software container, the `process.GlobalTag.connect` line makes the job read the condition data from the local `/cvmfs` area in the container. If it is left out, the condition data are read from predefined condition data servers and it may take longer. + +--- + **For 2016 simulated data**, for the special data science samples, the global tag is 80X_mcRun2_asymptotic_2016_TrancheIV_v8. **VM:** @@ -396,6 +436,8 @@ process.GlobalTag.snapshotTime = cms.string("9999-12-31 23:59:59.000") ### Heavy-ion related data +#### Run-1 + --- **For 2010 heavy-ion data**, the global tag is GR_R_39X_V6B. @@ -526,6 +568,8 @@ Define the global tag in the configuration file of the job: process.GlobalTag.globaltag = '::All' ``` +#### Run-2 + --- **For 2015 p-p reference data**, the global tag is 75X_dataRun2_v13. diff --git a/cernopendata/modules/fixtures/data/docs/cms-guide-for-research/cms-guide-for-research.md b/cernopendata/modules/fixtures/data/docs/cms-guide-for-research/cms-guide-for-research.md index 2af0047660..30b3c52d30 100644 --- a/cernopendata/modules/fixtures/data/docs/cms-guide-for-research/cms-guide-for-research.md +++ b/cernopendata/modules/fixtures/data/docs/cms-guide-for-research/cms-guide-for-research.md @@ -1,9 +1,11 @@ If you are interested in step-by-step instructions to start working with CMS Open Data, please consult these pages: -* [Install Virtual Machine](/docs/cms-virtual-machine-2011) or [Use a container](/docs/cms-guide-docker) -* [Get started with CMS Open Data](/docs/cms-getting-started-2011) +* [Install Virtual Machine](https://opendata.cern.ch/search?q=&f=tags%3AVM&f=experiment%3ACMS&l=list&order=desc&p=1&s=10&sort=mostrecent) or [Use a container](/docs/cms-guide-docker) +* Getting started with CMS [AOD Data](/docs/cms-getting-started-aod), for data collected during Run 1 of the LHC. +* Getting started with CMS [MiniAOD Data](/docs/cms-getting-started-miniaod) or [NanoAOD Data](/docs/cms-getting-started-nanoaod), for data collected during Run 2 of the LHC. +* Getting started with CMS [Heavy Ion Data](/docs/cms-getting-started-hi-2013-2015). -However, if you are interested in finding hints, tips and guidance for conducting a research-oriented analysis using CMS Open Data, please see our notes on this page. Note that possible solutions to frequently encountered issues can be found on [our page of known errors](/docs/cms-guide-troubleshooting). +This page offers hints, tips and guidance for conducting a research-oriented analysis using CMS Open Data. More detailed information can be found in the [CMS Open Data Guide](https://cms-opendata-guide.web.cern.ch/). --- @@ -11,108 +13,165 @@ However, if you are interested in finding hints, tips and guidance for conductin **I want to get a general introduction into HEP and CMS software and terminology, with a simplified event format.** -* Read the instructions related to [educational content](/docs/cms-guide-for-education) and follow the corresponding exercises. - +* Read the instructions related to our [educational content](/docs/cms-guide-for-education) and follow the corresponding exercises. **I want to learn about the terms under which I can access and use the CMS Open Data, and publish results obtained from them.** -* Go to ["Data preservation and open access policy"](/record/414) (if you are a CMS member, also see the internal document ["Rules for use of open access CMS data by individual members of CMS"](https://cms-docdb.cern.ch/cgi-bin/DocDB/ShowDocument?docid=12242)). - +* Go to the ["Data preservation and open access policy"](/record/414) (if you are a CMS member, also see the internal document ["Rules for use of open access CMS data by individual members of CMS"](https://cms-docdb.cern.ch/cgi-bin/DocDB/ShowDocument?docid=12242)). **I want to get inspiration for some potential physics topics.** -* A link with examples of potentially interesting physics topics and their relation to CMS Open Data might be added here soon. - +* See what others are doing with CMS Open Data! Papers citing DOI [10.7483/OPENDATA.CMS](https://inspirehep.net/literature?sort=mostrecent&size=25&page=1&q=references.reference.dois%3A10.7483%2FOPENDATA.CMS%2A) show a broad scope of usage for Open Data, including physics analyses, data science, and research tool development. **I want to learn about the nature of the CMS physics objects and the corresponding variables and terminology.** -* Go to ["CMS Physics Objects"](/docs/cms-physics-objects-2011). - ---- - -### Deciding which datasets to explore - -**I want to find out whether I should go for data from 2010 or 2011 (both are pp data at 7 TeV) or from 2012 (pp data at 8 TeV).** - -* The 2010 data have been released first; have fewer, smaller datasets with better low-pT tracking, low trigger thresholds, low pile-up and more/simpler analysis/validation examples; but have no MC. If you do not need MC or maximal statistics, you might want to try 2010 data first. -* The 2011/2012 data have more statistics, more diverse datasets, many associated MC sets, and a slightly more advanced VM environment. If you are immediately interested in maximal statistics and/or MC acceptance corrections you should go for 2011/2012 data. -* Information on the respective luminosities and pile-up rates vs time can be found in [public CMS luminosity information](https://twiki.cern.ch/twiki/bin/view/CMSPublic/LumiPublicResults#Multi_year_Collisions_Plots). -* If you want to try both datasets, you will need to use [the appropriate VMs](/search?page=1&size=20&tags=VM&experiment=CMS). - - -**I want to install the CMS software environment needed for access to and analysis of CMS Research level data.** - -* Install the appropriate virtual machine, [2010 VM](/record/250) for 2010 data, and [2011 VM](/record/252) for 2011/2012 data. -* As an alternative to a virtual machine you can try running the CMS software environment in a container by following [these instructions](/docs/cms-guide-docker). -* Go to ["Getting started with CMS 2010 open data"](/docs/cms-getting-started-2010) for 2010 or ["Getting started with CMS 2011 open data"](/docs/cms-getting-started-2011) for 2011/2012 data. - -**Note**: The 2010 (SL5) virtual machine will only work on 2010 data with CMSSW 4-2-8 (and other SLC5-based CMSSW releases). The 2011 (SL6) virtual machine will only work on 2011/2012 data and MC with CMSSW 5-3-32 (and other SLC6-based CMSSW releases). +* Check out the ["CMS Open Data Guide"](https://cms-opendata-guide.web.cern.ch/) as well as the pages describing CMS Physics Objects for [2011-2012 data](/docs/cms-physics-objects-2011) and for [2015 data](/docs/cms-physics-objects-2015). +**I want to follow a set of detailed tutorials to learn how to analyze CMS Open Data.** -**I want to produce some example physics distributions.** - -* Install the CMS software as in the previous item (for 2010 or 2011). -* Follow options A (inclusive di-muon spectrum analysis example directly from AOD) or B (two-/four-lepton analysis example with intermediate ntuples) in ["Getting started with CMS 2010 open data"](/docs/cms-getting-started-2010) or ["Getting started with CMS 2011 open data"](/docs/cms-getting-started-2011). +* Beginning in 2020, CMS has offered workshops targeting research use of Open Data. You can follow the lessons of previous workshops by [visiting this page](https://cms-opendata-guide.web.cern.ch/cmsOpenData/workshops/). --- -### Exploring the 2010 datasets - -**I want to find out which 2010 datasets exist, and how to get a feel for their content.** - -* Go to [2010 CMS primary datasets](/search?page=1&size=20&q=&type=Dataset&subtype=Collision&experiment=CMS&year=2010), -* choose a dataset, and read the comments. - - -**I also want to view some corresponding event displays.** - -* Go to [2010 CMS derived datasets of event display ("ig") type](/search?page=1&size=20&q=&type=Dataset&subtype=Derived&experiment=CMS&year=2010&file_type=ig), -* choose `Event display file derived from`… + the name of the CMS primary dataset you want (ZeroBias is known to be essentially empty). - -or, alternatively: - -* Load the [CMS event display](/visualise/events/cms), -* choose `Open File` → `Open Files from Web` → `2010`, and -* choose your dataset. - - -**I want to find out which 2010 dataset and/or analysis/validation example is most useful for my purpose.** +### Deciding which datasets to explore -* To learn how to do a muon analysis, follow "*I want to produce some example physics distributions*," (above) with either option A (recommended) or B, or try one of the relevant "*I want to run the examples used for validation of the 2010 datasets*," (further below). -- To learn how to do an electron analysis, follow "*I want to produce some first physics distributions*," (above) with option B, or try one of the relevant "*I want to run the examples used for validation of the 2010 datasets*," (below). -- To learn how to do a minimum-bias track analysis, try the MinimumBias example on "*I want to run the examples used for validation of the 2010 datasets*," (below). -- [More to come…] +CMS has released data proton collision data from Run 1 and Run 2, as well as heavy ion collision data from Run 1. + +High-energy proton collisions: + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
CollisionsEnergy (TeV)SimulationGetting StartedCMSSW version
proton-proton 201072010 simulationAOD dataCMSSW_4_2_8
proton-proton 201172011 simulationAOD dataCMSSW_5_3_32
proton-proton 201282012 simulationAOD dataCMSSW_5_3_32
proton-proton 2015132015 simulationMiniAOD dataCMSSW_7_6_7
proton-proton 2016132016 simulationMiniAOD data
NanoAOD data
CMSSW_10_6_30
Not required
+ +For Run 1 data, the 2010 datasets are smaller and offer a better environment for low-momentum, low-pileup studies. The 2011-2012 datasets are suitable for replicating CMS Run 1 physics results or performing new searches or studies at 7 - 8 TeV collision energy. Considering Run 2, the 2015 dataset is smaller than the 2011-2012 Run 1 datasets, but offered the first look at 13 TeV collisions and a much broader array of simulation. The 2016 13 TeV dataset (released as of 2024) has a similar luminosity to the Run 1 datasets, and offers a more advanced computing environment and new identification algorithms for Run 2. Information on the respective luminosities and pile-up rates vs time can be found in [public CMS luminosity information](https://twiki.cern.ch/twiki/bin/view/CMSPublic/LumiPublicResults#Multi_year_Collisions_Plots). + +Heavy-ion program: + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
CollisionsEnergy (TeV)SimulationGetting StartedCMSSW version
lead-lead 20102.762010-2011 Pb-Pb simulationPb-Pb 2010CMSSW_3_9_2_patch5\*
lead-lead 20112.762010-2011 Pb-Pb simulationPb-Pb 2011CMSSW_4_4_7\*
proton-proton 20112.76N/APb-Pb 2011CMSSW_4_4_7
proton-proton 20132.762013 p-p simulationp-Pb dataCMSSW_5_3_20
proton-lead 20135.022013 p-Pb simulationp-Pb dataCMSSW_5_3_20
proton-proton 20155.02N/Ap-Pb dataCMSSW_7_5_8_patch3
+ +\* The Pb-Pb simulation linked in these rows was produced later and should be analyzed using CMSSW_5_3_20. + +The Pb-Pb collisions from 2010 and 2011 are accompanied by "reference" proton-proton collisions at the same energy, collected during 2011 and 2013. The p-Pb collisions from 2013 are accompanied by referece proton-proton collisions collected during 2015. Some simulations have also been released that correspond to the heavy-ion collisions, as well as some of the reference collision data. --- -### Exploring the 2011-2012 datasets - -**I want to find out which 2011-2012 data and MC sets exist, and how to get a feel for their content.** +### Exploring event displays -* For collision data, go to [2011 CMS primary datasets](/search?page=1&size=20&q=&subtype=Collision&experiment=CMS&year=2011) or [2012 CMS primary datasets](/search?page=1&size=20&q=&subtype=Collision&experiment=CMS&year=2012) -* For MC, go to [2011 CMS simulated datasets](/search?page=1&size=20&q=&subtype=Simulated&experiment=CMS&year=2011) or [2012 CMS simulated datasets](/search?page=1&size=20&q=&subtype=Simulated&experiment=CMS&year=2012) -* choose a dataset, read the comments, and read also about [simulated dataset names](/docs/cms-simulated-dataset-names). - - -**I also want to to view some corresponding event displays.** - -* These are available for data only for the time being. -* Go to CMS derived datasets of event display ("ig") type for the [2011 data](/search?page=1&size=20&q=&subtype=Derived&experiment=CMS&year=2011&file_type=ig) or the [2012 data](/search?page=1&size=20&q=&subtype=Derived&experiment=CMS&year=2012&file_type=ig) , -* choose `Event display file derived from`… + the name of the CMS primary dataset you want (ZeroBias is known to be essentially empty). - -or, alternatively: +Visualizing CMS events is a very helpful way to get acquainted with the CMS detector and the features of different datasets. [Software](https://opendata.cern.ch/search?q=event%20display&f=experiment%3ACMS&f=type%3ASoftware&l=list&order=asc&p=1&s=10&sort=bestmatch) is provided to produce event display files from the Run 1 datasets, but many events are already available in this format for viewing on the web: * Load the [CMS event display](/visualise/events/cms), -* choose `Open File` → `Open Files from Web` → `2011` or `2012`, and -* choose your dataset. +* From the menu bar at the top, choose `Open File` → `Open Files from Web` → choose a year, and choose a dataset. +* Select a particular event from the list, and then other events can be explore using the arrow buttons in the menu bar. +* Various detector and/or physics features can be toggled on or off in the left-hand-side menu. +### Exploring example analyses -**I want to find out which 2011 or 2012 dataset and/or analysis/validation example is most useful for my purpose.** +Example analyses help demonstrate how analysts can process CMS data files to accomplish a real physics goal. Examples range from data validation exercises to full searches. The "Getting Started" pages linked in the table able all offer links to example analyses. -* Dedicated examples beyond those available in "Getting Started" can be found in [software](/search?page=1&size=20&type=Software&subtype=Analysis&experiment=CMS&year=2011&year=2011-2012), including Higgs-to-four-lepton analysis, jet tuple production and top cross-sections. Alternatively, start from a 2010 example and adjust to run on 2011 or 2012 data (see [the CMS troubleshooting guide](/docs/cms-guide-troubleshooting) for instructions). - - -* For more information on Monte Carlo, see below. +* [2010 proton-proton examples](https://opendata.cern.ch/search?q=&f=experiment%3ACMS&f=type%3ASoftware&f=year%3A2010&l=list&order=desc&p=1&s=10&sort=mostrecent) +* [2011 proton-proton examples](https://opendata.cern.ch/search?q=&f=experiment%3ACMS&f=type%3ASoftware&f=year%3A2011&l=list&order=desc&p=1&s=10&sort=mostrecent) +* [2012 proton-proton examples](https://opendata.cern.ch/search?q=&f=experiment%3ACMS&f=type%3ASoftware&f=year%3A2012&l=list&order=desc&p=1&s=10&sort=mostrecent) +* [Run 2 proton-proton examples](https://opendata.cern.ch/search?q=&f=experiment%3ACMS&f=type%3ASoftware&f=year%3A2015&f=year%3A2016&f=year%3A2017&f=year%3A2018&f=year%3A2019&l=list&order=desc&p=1&s=10&sort=mostrecent) +* [Heavy Ion examples](https://opendata.cern.ch/search?q=&f=experiment%3ACMS&f=type%3ASoftware&f=keywords%3Aheavy-ion%20physics&l=list&order=desc&p=1&s=10&sort=mostrecent) --- @@ -120,94 +179,50 @@ or, alternatively: **I want to find out how to use the trigger and trigger prescale information in the dataset I am interested in.** -* Go to [the guide to CMS trigger system](/docs/cms-guide-trigger-system). - +* Check [the guide to CMS trigger system](/docs/cms-guide-trigger-system). **I want to find out how to access the luminosity information for the dataset I am interested in and how to select "good data" only.** -* Check the [CMS luminosity information](/search?page=1&size=20&q=luminosity&type=Supplementaries&subtype=Luminosity), and +* Check the [CMS luminosity information for each year](/search?page=1&size=20&q=luminosity&type=Supplementaries&subtype=Luminosity), and * check the [list of validated runs](/search?page=1&size=20&q=%22CMS%20list%20of%20validated%20runs%22). - -**I want to find out whether I need condition data base information, and if so, how to access it.** - -* Condition data are needed on examples using e.g. jet energy corrections and trigger configuration information, many of the simpler analysis/validation examples do not need any additional corrections from condition database. -* Using condition data slows down data access, so use them only if really needed. If so: - * see the instructions in ["The Guide to the CMS condition database"](/docs/cms-guide-for-condition-database). - - **I want to find the luminosity of my dataset, possibly constrained by using specific triggers.** -* Please check [CMS luminosity information](/search?page=1&size=20&q=luminosity&type=Supplementaries&subtype=Luminosity), -* decide on the triggers you want to use, -* find out the runs/lumi sections in which these triggers were active and whether they were prescaled, -* overlap with the available CMS Open Data samples (run range) and with the selection in the list of validated runs. - * If not prescaled, sum up the luminosity for the surviving runs/lumi sections. - * If prescaled, life is more complicated. Find the prescales as in [the trigger example code](/record/5004) - ---- - -### Performing an analysis - -**I want to find more CMS software and data format documentation from public sources.** - -* This is strongly recommended for serious analysis, but is hard to navigate! -* Check the [CMS public Twiki](https://twiki.cern.ch/twiki/bin/view/CMSPublic/WebHome) or the CMS Fermilab website or use your favourite web-search engine. - - -**I want to learn about the published jet-analysis papers by the MIT group.** - -* See *Jet Substructure Studies with CMS Open Data*, A. Tripathee et al., Apr 19, 2017, MIT-CTP-4890, [arXiv:1704.05842](https://inspirehep.net/record/1593756), -* and *Exposing the QCD Splitting Function with CMS Open Data*, A. Larkoski et al., Apr 17, 2017, MIT-CTP-4891, [arXiv:1704.05066](https://inspirehep.net/record/1591972). +* Check the [Guide to calculate luminosity](https://opendata.cern.ch/docs/cms-guide-luminosity-calculation) +**I want to find out whether I need condition data base information, and if so, how to access it.** -**I want to run the examples used for validation of the 2010 datasets within my setup…** - -* … for the MinimumBias, Commissioning, Mu or MuMonitor datasets: - * Go to [Validation software](/search?page=1&size=20&q=&subtype=Validation&type=Software&year=2010) - * choose and execute the corresponding Validation code. -* … for the Multijet dataset (see also [here](http://hep.caltech.edu/cms/opendata/)): - * choose and execute ["Razor filter and analyzer for SUSY searches"](/record/553). -* … for the Electron (or Mu) dataset: - * choose and execute ["Software to preprocess the CMS 2010 Muon and Electron datasets for the two-lepton/four-lepton analysis example of CMS open data"](/record/200), then - * choose ["Two-lepton/four-lepton analysis example of CMS 2010 open data"](/record/101) and compare PAT-tuples from the previous to those linked therein, or execute it on your new PAT tuples. -* … for the ZeroBias dataset: - * Not useful, no validation needed. -* … for the Jet, MuOnia, BTau, Photon, JetMETTaumonitor, METFwd datasets: - - Validation not yet available (partially in preparation). - - -**I want to backup my code, or import some external code.** - -* You can use `scp` from and to your host from within the VM. +* Condition data are needed for examples using e.g. jet energy corrections and trigger configuration information, many of the simpler analysis examples do not need any additional corrections from the conditions database. +* The most recent CMSSW containers contain the conditions database information needed for the relevant year's data, and example analysis frameworks such as the [Physics Object Extractor Tool](https://opendata.cern.ch/search?q=PhysObjectExtractorTool&f=type%3ASoftware%2Bsubtype%3ATool&l=list&order=asc&p=1&s=10&sort=bestmatch) demonstrate how to access this information. +* More information is available in the ["Guide to the CMS condition database"](/docs/cms-guide-for-condition-database). --- -### Monte Carlo +### Using simulation -**How do I interpret the MC set names?** +**How do I interpret the simulated dataset names?** * Check [CMS Simulated Dataset Names](/docs/cms-simulated-dataset-names). +**I want to find the generator cross section of a particular simulation.** -**I want to find the effective luminosity of my MC set.** - -* Information will be added to the portal. -* Generically: divide MC cross-section (next item) times matching efficiency times filter efficiency by the number of events. +* Check [CMS Simulation cross sections](/docs/cms-guide-cross-sections). -**I want to find the generator cross section of a particular MC set.** +**I want to find the effective luminosity of my simulated dataset.** -* To be documented. -* On some MC sets, the following might work (reliability of information not guaranteed): open the ROOT file, create TBrowser and navigate to `Runs` → `GenRunInfoProduct_generator__SIM.` → `GenRunInfoProduct_generator__SIM.obj` → `InternalXSec` → `value_`. +* Effective luminosity = (cross section) $\times$ (generator matching efficiency, if applicable) $\times$ (generator filter efficiency, if applicable) / (Number of positive-weight events - Number of negative-weight events). +* Find more information about using simulation in the [CMS Open Data Guide](https://cms-opendata-guide.web.cern.ch/analysis/backgrounds/). --- -### Further information / Contact us +### Contact us **I want information that is not documented here and elsewhere on the [CERN Open Data portal](http://opendata.cern.ch/).** -* Kindly contact <[opendata-support@cern.ch](mailto:opendata-support@cern.ch)> +* Please check the [CMS Open Data Guide](https://cms-opendata-guide.web.cern.ch). +* Kindly reach out on the [CERN Open Data Forum](https://opendata-forum.cern.ch/) and tag "CMS" in your message. **I ran into a problem and need help!** * Please check [our page related to known errors](/docs/cms-guide-troubleshooting). +* Kindly reach out on the [CERN Open Data Forum](https://opendata-forum.cern.ch/) and tag "CMS" in your message. \ No newline at end of file diff --git a/cernopendata/modules/fixtures/data/docs/cms-guide-pileup-simulation/cms-guide-pileup-simulation.json b/cernopendata/modules/fixtures/data/docs/cms-guide-pileup-simulation/cms-guide-pileup-simulation.json index 56529ee53d..717738befc 100644 --- a/cernopendata/modules/fixtures/data/docs/cms-guide-pileup-simulation/cms-guide-pileup-simulation.json +++ b/cernopendata/modules/fixtures/data/docs/cms-guide-pileup-simulation/cms-guide-pileup-simulation.json @@ -16,7 +16,7 @@ "CMS" ], "short_description": { - "content": "Monte Carlo simulation of pile-up is controlled by the code and configuration files of the CMSSW package SimGeneral/MixingModule. An input distribution is specified for each set of production samples which is supposed to represent the distribution of the mean number of interactions seen during data-taking." + "content": "At the LHC, many collisions occur simultaneously within one proton-proton bunch crossing. These additional interactions, beyond the primary interaction, from the current bunch crossing are called in-time pileup." }, "slug": "cms-guide-pileup-simulation", "tags": [ diff --git a/cernopendata/modules/fixtures/data/docs/cms-guide-pileup-simulation/cms-guide-pileup-simulation.md b/cernopendata/modules/fixtures/data/docs/cms-guide-pileup-simulation/cms-guide-pileup-simulation.md index bfd49788f4..d9247250d6 100644 --- a/cernopendata/modules/fixtures/data/docs/cms-guide-pileup-simulation/cms-guide-pileup-simulation.md +++ b/cernopendata/modules/fixtures/data/docs/cms-guide-pileup-simulation/cms-guide-pileup-simulation.md @@ -1,45 +1,105 @@ -## Description +## Introduction -Monte Carlo simulation of pile-up is controlled by the code and configuration files of the [CMSSW](/search?page=1&size=20&q=CMSSW&type=Software) package `SimGeneral/MixingModule`. An input distribution is specified for each set of production samples which is supposed to represent the distribution of the mean number of interactions seen during data-taking. +At the LHC, many collisions occur simultaneously within one proton-proton bunch crossing. These additional interactions, beyond the "primary" interaction, from the current bunch crossing are called "in-time pileup". The detector response may be affected by pileup interactions from the current brunch crossing as well as nearby bunch crossings. The interactions from the nearby bunch crossings are called "out-of-time pileup". We need to model the additional pileup collisions in CMS simulation. -## Introduction +Monte Carlo simulation of pile-up is controlled by the code and configuration files in the `SimGeneral/MixingModule` of the CMSSW software. The simulation proceeds as follows: -Monte Carlo simulation of pileup is controlled by the code and configuration files of the [CMSSW](/search?page=1&size=20&q=CMSSW&type=Software) package `SimGeneral/MixingModule`. An input distribution (histogram) is specified for each set of production samples which is supposed to represent the distribution of the mean number of interactions seen during data-taking. The simulation proceeds as follows: +1. A distribution of the mean number of interactions per bunch crossing is created for a given year of data taking, as seen below. A value chosen from this distribution is assigned as the mean number of interactions to be simulated in an event, for all bunch crossings. This value is recorded as the "true number of interactions" for the event. This sets the instantaneous luminosity to be simulated for all of the bunch crossings in that event. -1. For each event, the mean number of interactions per crossing is chosen from the input histogram. This sets the instantaneous luminosity to be simulated for all of the bunch crossings in that event. For each event, this value is recorded as the "true" number of interactions. (`TrueNumInteractions`) +2. The number of interactions per bunch crossing (in-time and out-of-time) in the event is randomly sampled from a Poisson distribution with its mean equal to the value chosen in (1). This determines how many pileup interactions are added to the simulated event. This value is recorded as the "number of pileup interactions" in the event. -2. For each bunch crossing, both in- and out-of-time, the number of interactions is randomly sampled from a poisson distribution with a mean equal to the value chosen in (1). Note that this implies that all bunches have the same instantaneous luminosity, rather than allowing for bunch-to-bunch luminosity variation. In practice, the spread of bunch-by-bunch luminosities is much smaller than the poisson distribution, so this effect is negligible. One might evolve the simulation to include such features as the beginning or end of bunch trains, where the out-of-time pileup will have a significantly different luminosity structure (i.e., there is none, either before or after a given event). Since the bunch trains are quite long, this effect of ignoring these variations is likely to be negligible as well. The number of interactions that is actually included in each bunch crossing is also recorded. (`num_PU_vertices_`). +Note that applying the same mean number of interactions to all the bunch crossings in an event imposes that all bunches have the same instantaneous luminosity. Neglecting bunch-to-bunch luminosity variations is a negligible effect: in practice, the spread of bunch-by-bunch luminosities is much smaller than the spread of the Poisson distribution, and the long bunch trains used in the LHC make the effect of ignoring any variations from the bunch-train structure negligibly small as well. -## Pileup Distributions from Data +## Pileup distributions -The pileup distributions measured from data are available in [the CMS Luminosity information page](https://twiki.cern.ch/twiki/bin/view/CMSPublic/LumiPublicResults). +#### Measured from data -## Monte Carlo Pileup Distributions +The pileup distributions measured from data are available in the [CMS Luminosity information page](https://twiki.cern.ch/twiki/bin/view/CMSPublic/LumiPublicResults). -The "ideal" distributions input for each year's Monte Carlo production samples are catalogued on [this page](https://twiki.cern.ch/twiki/bin/view/CMSPublic/Pileup_MC_Gen_Scenarios), which contains the actual numerical contents of each bin represented in the plots below. +#### Used in Monte Carlo production -### 2011 +The numerical contents of the estimated pileup distributions used in the MC productions can be found on [this page](https://twiki.cern.ch/twiki/bin/view/CMSPublic/Pileup_MC_Gen_Scenarios). The distribution varies for each year. The plots below are made from the numerical values (corresponding to each year's pileup scenario) provided on that page. The x-axis of the histograms below are "mean number of interactions per bunch crossing". -For the 2011 Data, the distribution shown here was used to generate the Monte Carlo events. It is matched directly to that observed in the data for the 2011 running, so little or no reweighting should be necessary to achieve good agreement between data and simulation as far as pileup is concerned. +**2011** -The pileup distribution used to generate 2011 Monte Carlo events.: +For the 2011 Data, the distribution shown here was used to generate the Monte Carlo events. It is matched directly to that observed in the data for the 2011 running, so little or no reweighting should be necessary to achieve good agreement between data and simulation as far as pileup is concerned.

-

+

-### 2012 +**2012** -For the 2012 data, the distribution shown here was used to generate the Monte Carlo events. On the Twiki page referenced above, this is the S10 distribution. Unlike 2011, this distribution is not an exact match to the data, so reweighting of the Monte Carlo samples is required in order to obtain good agreement. -Pileup distribution used to generate the 2012 Monte Carlo samples: +For the 2012 data, the distribution shown here was used to generate the Monte Carlo events. On the webpage referenced above, this is the S10 distribution. Unlike 2011, this distribution is not an exact match to the data, so reweighting of the Monte Carlo samples is required in order to obtain good agreement.

-

+

-### 2015 +**2015** For the 2015 data, the distribution measured from the [2012 collision data](https://twiki.cern.ch/twiki/bin/view/CMSPublic/LumiPublicResults#2012_proton_proton_8_TeV_collisi), scaled by 4/5 to correspond to the estimated mean number of interactions per crossing in 2015, was used to generated the Monte Carlo events. -## Disclaimer +**2016** + +For the 2016 data, the distribution shown here was used to generate the Monte Carlo events. This distribution is not an exact match to the data, so reweighting of the Monte Carlo samples is required in order to obtain good agreement. + +

+

+ +## Access Pileup Information Stored in Datasets + +#### AOD and MiniAOD + +The Monte Carlo information about pileup is available in the form of a vector of `PileupSummaryInfo` objects for the different bunch crossings. In AOD, the collection is `addPileupInfo`, which has detailed information for both in-time and out-of-time bunch crossings. In MiniAOD, the collection is called `slimmedAddPileupInfo`, and has been slimmed by not saving detailed information for the out-of-time bunch crossings. + +The information is accessed using two functions defined in `SimDataFormats/PileupSummaryInfo/` of the CMSSW software: + +- `getTrueNumInteractions()` retrieves the true mean number of the Poisson distribution, from which the number of interactions in each bunch crossing of the event has been sampled. +- `getPU_NumInteractions()` retrieves the actual number of interactions that have been added. + +Here's an example of using these two functions. In an EDAnalyzer, the pileup collection can be accessed following this example. If you are unfamiliar with EDAnalyzers, check how to use an EDAnalyzer to analyze the CMS data in [AOD format](/doc/cms-getting-started-aod) or in [MiniAOD format](/doc/cms-getting-started-miniaod) first. + +At the top of the EDAnalyzer's `MyAnalyzer.cc` file, include the pileup info header file: +``` +#include "SimDataFormats/PileupSummaryInfo/interface/PileupSummaryInfo.h" +``` + +In the class definition of the EDanalyzer, define a "token" in the member data section: +``` +// ----------member data --------------------------- +edm::EDGetTokenT> PileupToken; +``` + +In the constructor function for the EDAnalyzer, set up access to the pileup collection using the token: +``` +MyAnalyzer::MyAnalyzer(const edm::ParameterSet& iConfig) +{ + edm::InputTag PileupTag("slimmedAddPileupInfo"); // "addPileupInfo" for AOD files + PileupToken = consumes>(PileupTag); +} +``` + +Now, in the main `analyze` function of the EDAnalyzer, access the pileup info as follows: +``` +void MyAnalyzer::analyze(const edm::Event& iEvent, const edm::EventSetup& iSetup) +{ + + int NumTrueInts = -1; + int NumPUInts = -1; + + edm::Handle> PileupInfo; + event.getByToken(PileupToken, PileupInfo); + + for(std::vector::const_iterator iPU = PileupInfo->begin(); iPU != PileupInfo->end(); iPU++){ + int BX = iPU->getBunchCrossing(); + if(BX == 0){ // "0" is the in-time crossing. Negative are early crossings. Positive are late. + NumTrueInts = PVI->getTrueNumInteractions(); + NumPUInts = PVI->getPU_NumInteractions(); + } + } +} +``` + +#### NanoAOD +- The true mean number of the Poisson distribution, from which the number of interactions in each bunch crossing in the event has been sampled, is stored in the branch `Pileup_nTrueInt`. -The open data are released under the [Creative Commons CC0 waiver](http://creativecommons.org/publicdomain/zero/1.0/). Neither CMS nor CERN endorse any works, scientific or otherwise, produced using these data. -All releases will have a unique DOI that you are requested to cite in any applications or publications. +- The number of interactions that have been added to the event in the current bunch crossing is stored in the branch `Pileup_nPU`. \ No newline at end of file diff --git a/cernopendata/modules/fixtures/data/docs/cms-guide-xsec/cms-guide-xsec.json b/cernopendata/modules/fixtures/data/docs/cms-guide-xsec/cms-guide-xsec.json new file mode 100644 index 0000000000..c28f370f82 --- /dev/null +++ b/cernopendata/modules/fixtures/data/docs/cms-guide-xsec/cms-guide-xsec.json @@ -0,0 +1,33 @@ +[ + { + "body": { + "content": "cms-guide-xsec.md", + "format": "md" + }, + "collections": [ + { + "experiment": "CMS" + }, + { + "primary": "VM" + } + ], + "experiment": [ + "CMS" + ], + "short_description": { + "content": "The number of events in the MC datasets do not match the number of events we expect to observe for each process, so we need to normalize the simulation to correspond to some cross section..." + }, + "slug": "cms-guide-xsec", + "tags": [ + "Getting Started" + ], + "title": "Standard Model cross-sections for CMS analyses", + "type": { + "primary": "Documentation", + "secondary": [ + "Guide" + ] + } + } +] diff --git a/cernopendata/modules/fixtures/data/docs/cms-guide-xsec/cms-guide-xsec.md b/cernopendata/modules/fixtures/data/docs/cms-guide-xsec/cms-guide-xsec.md new file mode 100644 index 0000000000..cdc61b9766 --- /dev/null +++ b/cernopendata/modules/fixtures/data/docs/cms-guide-xsec/cms-guide-xsec.md @@ -0,0 +1,201 @@ +The number of events in the simulated datasets do not match the number of events we expect to observe for each process, so we need to normalize the simulation to correspond to some cross section. Cross sections evaluated at next-to-leading order (NLO) or next-to-next-to-leading order (NNLO) in perturbative QCD are preferred, because they are more accurate. However, leading-order simulation remains the default for many SM processes, so higher-order cross sections cannot be extracted from the simulation itself. This page documents cross sections commonly used in CMS for Run 1 and Run 2 datasets. + +## Run 1 + +Selected SM cross section values for Run 1 datasets can be found in the following tables. More details about these cross sections are available [here](https://twiki.cern.ch/twiki/bin/view/CMSPublic/StandardModelCrossSections).
+ +Higher-order top quark cross sections are available from the LHC Physics Working Group for all LHC energies: + +- Top quark pair production at [NNLO](https://twiki.cern.ch/twiki/bin/view/LHCPhysics/TtbarNNLO) +- Single top quark production at [NLO](https://twiki.cern.ch/twiki/bin/view/LHCPhysics/SingleTopRefXsec) and at [NNLO](https://twiki.cern.ch/twiki/bin/view/LHCPhysics/SingleTopNNLORef)
+ +### 7 TeV + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
Process
Generator/Source
Phase space cuts
Order
Final state
Cross section (pb)
Uncertainty (pb):
Scale unc. (PDF unc.)
W+ FEWZ-- NNLOW->lv, l=e,m,t18456±233 (±850)
W- FEWZ-- NNLOW->lv, l=e,m,t12858 ±174 (±654)
Total W FEWZ-- NNLOW->lv, l=e,m,t31314 ±407 (±1504)
Z/a* (20) FEWZm(ll)>20GeV NNLOZ -> ll 4998±34 (±270)
Z/a* (50) FEWZm(ll)>50GeV NNLOZ -> ll 3048±34 (±128)
Z/a* (60-120)FEWZ60 < m(ll) < 120 GeVNNLOZ -> ll 2916±34 (±122)
W+cbar MCFM-- NLO Inclusive 1718±157
W-c MCFM-- NLO Inclusive 1910±164
Total Wc MCFM-- NLO Inclusive 3628±227
W+b bbar MCFM-- LO Inclusive 22.1±4.4
W-b bbar MCFM-- LO Inclusive 13.2±2.5
Total Wb bbarMCFM-- LO Inclusive 35.3±5.1
Z/a*b bbar MCFMm(ll) > 20 GeV LO Inclusive 67.3±18.8
W+W- MCFM-- NLO Inclusive 43 ±1.5
W+Z/a* MCFMm(ll) > 40 GeV NLO Inclusive 11.8±0.6
W-Z/a* MCFMm(ll) > 40 GeV NLO Inclusive 6.4 ±0.4
Total WZ/a* MCFMm(ll) > 40 GeV NLO Inclusive 18.2±0.7
Z/a* Z/a* MCFMm(ll) > 40 GeV NLO Inclusive 5.9 ±0.15
ttbarW -- -- NLO Inclusive 0.1473 ±0.0155
ttbarZ -- -- NLO Inclusive 0.1369 ±0.029 +
+ +### 8 TeV + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + + +
Process
Generator/Source
Phase space cuts
Order
Final state
Cross section (pb)
Uncertainty (pb):
Scale unc. (PDF unc.)
W+ FEWZ 3.1-- NNLOW->μν 7213.4 +45.3 -21.3 (±241.3)
W- FEWZ 3.1-- NNLOW->μν 5074.7 +33.8 -18.3 (±188.3)
Total W FEWZ 3.1-- NNLOW->μν 12234.4 +79.0 -39.7 (±414.7)
Z/a*(20) FEWZ 3.1m(ll)>20 GeV NNLOZ -> μμ 1966.7 +19.8 -13.7 (±87.7)
Z/a* (50) FEWZ 3.1m(ll)>50 GeV NNLOZ -> μμ 1177.3 +5.9 -3.6 (±38.8)
Z/a* (60-120) FEWZ 3.160 < m(ll) < 120 GeVNNLOZ -> μμ 1129.2 +5.5 -2.6 (±37.5)
W+cbar MCFM -- NLO Inclusive 2423.5
W+cbar MCFM -- NLO Inclusive 2624.6
Total Wc MCFM -- NLO Inclusive 5048.1
Total Wb bbar aMC@NLO -- NLO Inclusive 377.4 +19.5% -16.8%
Z/a*b bbar MCFM m(ll) > 50 GeV LO Inclusive 76.75
Total WZ/a* MCFM m(ll) > 12 GeV NLO Inclusive 33.21 (CTEQ)
33.85 (MSTW)
33.72 (NNPDF)
ttbarW MCFM -- NLO Inclusive 0.232 ±0.067 (±0.03)
ttbarZ NLO -- NLO Inclusive 0.2057 +0.019 -0.024
tqZ; q!=b aMC@NLO m(ll) > 50 GeV NLO Z->leptons 0.02450 +3.3% -2.6%
tbZ aMC@NLO m(ll) > 50 GeV NLO Z->leptons 0.0114 +3.3% -2.6%
WWW aMC@NLO -- NLO Inclusive 8.058e-02 +4.7% -3.9%
WWZ aMC@NLO -- NLO Inclusive 5.795e-02 +5.6% -4.6%
WZZ aMC@NLO -- NLO Inclusive 1.968e-02 +6.0% -4.9%
ZZZ aMC@NLO -- NLO Inclusive 5.527e-03 +2.7% -2.4%
tttt aMC@NLO -- NLO Inclusive 9.144e-04 +36.3%, -27.0%
W+ W- MCFM 6.60 NLO W->eν W->eν0.6472 ±0.0231 (±0.0266)
W+ Z/a* MCFM 6.6m(l+l-) > 12 GeV NLO W->μν Z->ee0.0748 ±0.0025 (±0.0029)
W+ Z/a* MCFM 6.6m(l+l-) > 40 GeV NLO W->μν Z->ee0.0535 ±0.0018 (±0.0028)
W- Z/a* MCFM 6.6m(l+l-) > 12 GeV NLO W->μν Z->ee0.0446 ±0.0021 (±0.0018)
W- Z/a* MCFM 6.6m(l+l-) > 40 GeV NLO W->μν Z->ee0.0305 ±0.0014 (±0.0014)
Z/a* Z/a* MCFM 6.6both dileptonic
m(l+l-) > 12 GeV
NLO Z->μμ Z->ee 0.0385 ±0.0011 (±0.0011)
Z/a* Z/a* MCFM 6.6both dileptonic
m(l+l-) > 40 GeV
NLO Z->μμ Z->ee 0.0185 ±0.0007 (±0.0007)
Z/a* Z MCFM 6.6m(l+l- from Z/a*) > 12 GeV NLO Z->ee Z->νν 0.1318 ±0.0040 (±0.0067)
Z Z MCFM 6.6both dileptonic
m(l+l-) > 1 GeV
NLO Z->ee Z->μμ 0.0173 ±0.0067 (±0.0007)
+
+ +## Run 2 + +### Calculate cross sections using GenXSecAnalyzer + +For Run2, the [GenXSecAnalyzer tool](https://github.com/cms-sw/cmssw/blob/CMSSW_7_6_X/GeneratorInterface/Core/plugins/GenXSecAnalyzer.cc) is available to compute cross section from an existing MC sample in [MiniAOD format](/docs/cms-getting-started-miniaod). It retrieves information from collections called [GenLumiInfoProduct](https://github.com/cms-sw/cmssw/blob/CMSSW_7_6_X/SimDataFormats/GeneratorProducts/interface/GenLumiInfoProduct.h) and [GenFilterInfo](https://github.com/cms-sw/cmssw/blob/CMSSW_7_6_X/SimDataFormats/GeneratorProducts/interface/GenFilterInfo.h) to compute averaged cross sections over all the input luminosity blocks. + +**Many SM simulations corresponding to Run 2 data have the output of this analyzer available on the record page.** + +The following instructions show how to compute a cross section from a MiniAOD sample. This example is given for a 2015 +MiniAOD dataset using CMSSW_7_6_7, but the commands can be adapted for later MiniAOD samples by using the corresponding +CMSSW release and updating the input file or dataset names. + +Setup the CMS environment by following the [instructions for MiniAOD](/docs/cms-getting-started-miniaod). + +Inside the `CMSSW_7_6_7/src` directory, fetch a configuration file for the `GenXSecAnalyzer`: +``` +curl https://raw.githubusercontent.com/cms-sw/genproductions/master/Utilities/calculateXSectionAndFilterEfficiency/genXsec_cfg.py -o genXSecAnalyzer_cfg.py +``` + +Examine the configuration file with your preferred editor. Within the configuration file, the `maxEvents` setting +controls the maximum number of events passed to the GenXSecAnalyzer. Set it to `-1` if you would like to use all the events: +``` +process.maxEvents = cms.untracked.PSet( + input = cms.untracked.int32(options.maxEvents) +) +``` + +The `source` setting specifies the names of the root files to be used: +``` +process.source = cms.Source ("PoolSource", + fileNames = cms.untracked.vstring(options.inputFiles), + secondaryFileNames = secFiles +) +``` + +You may specify `inputFiles` and `maxEvents` and run the script in command line: +``` +cmsRun genXSecAnalyzer_cfg.py inputFiles="file:root://eospublic.cern.ch//eos/opendata/cms/mc/RunIIFall15MiniAODv2/QCDJets_flat_pythia_shifted15mmvertex/MINIAODSIM/PU25nsData2015v1_Shifted15mmCollision2015_76X_mcRun2_asymptotic_v12-v1/60000/00D4D020-59B8-E511-8D6D-A0000420FE80.root" maxEvents=10 +``` + +Here we use a root file from 2015 QCD MC sample and set the maximum number of events to 10. +The printout should look like this: +``` +------------------------------------ +GenXsecAnalyzer: +------------------------------------ +Before Filtrer: total cross section = 1.887e+09 +- 7.281e+07 pb +Filter efficiency (taking into account weights)= (3.38384) / (3.38384) = 1.000e+00 +- 0.000e+00 +Filter efficiency (event-level)= (200) / (200) = 1.000e+00 +- 0.000e+00 +After filter: final cross section = 1.887e+09 +- 7.281e+07 pb + +============================================= +``` + +Depending on the type of simulation, the analyzer will present different information. The most common values are: +* Before matching: the cross section before jet matching and any filter. +* After matching: the cross section after jet matching BUT before any filter. +* Filter efficiency: the efficiency of any filter. +* After filter: the cross section after jet matching and additional filters are applied. This is your final cross section. + +To compute the cross section of *QCDuubar_Pt-15to3000_TuneZ2star_Flat_13TeV_pythia6* for 2015 data using **all the files** in this sample, find the link to the filelist on this dataset's [record](https://opendata.cern.ch/record/18392). + +In `CMSSW_7_6_7/src` (or `CMSSW_10_6_30/src` for 2016 datasets), download the filelist using its URL: +``` +curl https://opendata.cern.ch/record/18392/files/CMS_mc_RunIIFall15MiniAODv2_QCDuubar_Pt-15to3000_TuneZ2star_Flat_13TeV_pythia6_MINIAODSIM_PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1_60000_file_index.txt -o filelist.txt +``` + +Create a python script `compute_xsec.py` with the following code that will read the file list and provide all the files +as an argument to the analyzer: +``` +import os + +# parameters to EDIT +inputFilelist = "filelist.txt" +maxEvents = "10" # You may increase maxEvents for a better estimation (e.g. set to -1) +outfileName = "xsec_QCDuubar_Pt-15to3000.log" + +# get inputFiles +filelist = open(inputFilelist, 'r').readlines() +inputFiles = "" +for rootfile in filelist: + if('root' in rootfile): + inputFiles += ' inputFiles='+rootfile + ' ' + +# compute cross section +command = 'cmsRun genXSecAnalyzer_cfg.py {} maxEvents={} 2>&1 | tee {}'.format(inputFiles, maxEvents, outfileName) +os.system(command) +``` + +In the CMS environment (make sure you have executed `cmsenv` if using a VM), run: +``` +python compute_xsec.py +``` + +### 13 TeV higher-order cross sections + +Higher order top quark cross sections are available from the LHC Physics Working Group for all LHC energies: + +- Top quark pair production at [NNLO](https://twiki.cern.ch/twiki/bin/view/LHCPhysics/TtbarNNLO) +- Single top quark production at [NLO](https://twiki.cern.ch/twiki/bin/view/LHCPhysics/SingleTopRefXsec) and at [NNLO](https://twiki.cern.ch/twiki/bin/view/LHCPhysics/SingleTopNNLORef)
+ +A table of further higher-order cross sections for other processes will be added when available. + diff --git a/cernopendata/modules/fixtures/data/docs/cms-virtual-machine-cc7/cms-virtual-machine-cc7.json b/cernopendata/modules/fixtures/data/docs/cms-virtual-machine-cc7/cms-virtual-machine-cc7.json new file mode 100644 index 0000000000..edc34dc602 --- /dev/null +++ b/cernopendata/modules/fixtures/data/docs/cms-virtual-machine-cc7/cms-virtual-machine-cc7.json @@ -0,0 +1,36 @@ +[ + { + "body": { + "content": "cms-virtual-machine-cc7.md", + "format": "md" + }, + "collections": [ + { + "experiment": "CMS" + }, + { + "primary": "VM" + }, + { + "year": "2016" + } + ], + "experiment": [ + "CMS" + ], + "short_description": { + "content": "The CMS-specific VM includes the ROOT framework and CMSSW. Follow the instructions below to setup a CERN Virtual Machine on your computer for Run2 CMS MiniAOD Open Data. Then, go to Getting Started with CMS data." + }, + "slug": "cms-virtual-machine-cc7", + "tags": [ + "VM" + ], + "title": "CMS CC7 Virtual Machines: How to install", + "type": { + "primary": "Documentation", + "secondary": [ + "Guide" + ] + } + } +] diff --git a/cernopendata/modules/fixtures/data/docs/cms-virtual-machine-cc7/cms-virtual-machine-cc7.md b/cernopendata/modules/fixtures/data/docs/cms-virtual-machine-cc7/cms-virtual-machine-cc7.md new file mode 100644 index 0000000000..7a7a2b350d --- /dev/null +++ b/cernopendata/modules/fixtures/data/docs/cms-virtual-machine-cc7/cms-virtual-machine-cc7.md @@ -0,0 +1,112 @@ +The CMS-specific VM includes the [ROOT framework](http://root.cern.ch/) and [CMSSW](http://cms-sw.github.io/). Follow the instructions below to set it up on your computer for Run2 CMS MiniAOD open data from 2016 - 2018. Then, go to [Getting Started with CMS MiniAOD data][getstartedcms] + +1. [How to install a CERN VM](#vbox) +2. [How to set up the CMSSW working area](#test) +3. [Issues & Limitations](#issue) + +## Step 1: How to install a CERN Virtual Machine + +### Installing VirtualBox + +VirtualBox is a free, open source and multiplatform application to run virtual machines: you can [download][installVB] the package for your platform from the Downloads page. + +You will need administrative ("root") privileges on every platform to perform the installation of VirtualBox. + +Note: the latest version of VirtualBox tested with this CMS-specific CernVM image is 7.0.4. If you have troubles with other versions of VirtualBox, pick that one: the full history of VirtualBox versions is available [on a different page][installVB2]. + + +### Downloading and Creating a Virtual Machine + +Download the CMS-specific CernVM image as OVA file from [CMS CC7 VM Image, for CMS MiniAOD open data from 2016 - 2018][cmsvmimagecc7]. + +By double clicking the downloaded file, VirtualBox imports the image with default settings. In VirtualBox version 6 or later, you need to unselect "import disks as VDI" on the initial import screen. Before launching the image, change the network settings: select the image from the left bar of the VirtualBox window, go to Settings and select Networks and change the network setting for network adaptor 2 to "NAT". Then, launch the CMS-specific CernVM, which boots into the graphical user interface and sets up the CMS environment. Then, be patient, the boot will take a while. + + +## Step 2: How to set up the CMSSW working area + +### Set up the CMS environment + +In the "CMS-OpenData-1.6.0" VM, open a terminal from the "CMS Shell" icon from the desktop as shown in the figure (note that the X terminal emulator from an icon bottom-left of the VM screen opens a shell with an operating system that might get updated to become incompatible with the CMS software release to be used but can be used e.g. for the git commands or ROOT). + + + +Build the local release area (the directory structure) for CMSSW. This only needs to be run once (note that it may take a while): + +``` +cmsrel CMSSW_10_6_30 +``` + +Change to the ```CMSSW_10_6_30/src/``` directory: + +``` +cd CMSSW_10_6_30/src/ +``` + +Set up the CMS environment with: + +``` +cmsenv +``` + +Then, head straight to [Getting Started with CMS MiniAOD Open Data](/docs/cms-getting-started-miniaod#data) to see how to acces data. + + +## Known Issues & Limitations + +### Known Issues FAQ + +**Question:** The following error message appears when the Virtual Machine is started: "Could not start the machine CMS Open Data because the following physical network interfaces were not found: vboxnet0 (adapter 2). You can either change the machine's network settings or stop the machine." + +> **Answer:** Change the Network settings for adapter 2 from "Host-only Adapter" to "NAT". The VM should then start correctly. + + +**Question:** What is the root password for the CMS Open Data VM? + +> **Answer:** The root password for the CMS Open Data VM is password, but if you need it when starting the VM, something has most likely gone wrong. + +**Question:** The CMS Open Data VM does not open correctly + +> **Answer:** In some versions of VirtualBox, it has happened that the CMS Open Data VM does not open correctly. This was the case for example for VirtulBox 5.0.32, but more recent versions from the VirtualBox website have been tested and are working properly. Note that it can take a while to launch the CMS Open Data VM for the first time. + +**Question:** In VirtualBox version 6, importing the CMS Open Data VM gives an error message ' element in OVF contains a medium attachment for the disk image but the OVF describes no such image.' + +> **Answer:** Uncheck the default option "Import hard drives as VDI" in the VirtualBox import menu. It may also happen that the folder in which VirtualBox writes the images ('/users/[username]/VirtualBox VMs') does not get created. In this case you can create it manually. + +**Question:** When/after installing CERN VM, I get a message that my VM uses too much memory + +> **Answer:** Reduce the memory allocated to VirtualBox by clicking on System in the VirtualBox graphical user interface and adjust the base memory with the sliding bar. + + + +**Question:** On Ubuntu running the latest version of VirtualBox, an error appears when opening the CMS-specific virtual machine: the message is about a missing path to a definition file. + +> **Answer:** To fix this, open one of the (non-CMS-specific) CernVMs first, after which the CMS-specific one should load without the error message. + + + +**Question:** The VM does not inherit the keyboard layout of the host machine. + +> **Answer:** The layout can be changed by using setxkbmap from a terminal inside the Virtual Machine. For example a user with a Swiss keyboard with French variant would type ```setxkbmap 'ch(fr)'``` in the terminal and a user with a Finnish keyboard would type ```setxkbmap fi```. This can also be solved by using the GUI, which can be launched either from the graphical menu in the lower left corner (Preferences → Keyboard) or by typing in the console: xfce4-keyboard-settings. In the Layout tab it is possible to change the keyboard model and the layout. If you wish to keep these settings after reboot, you should delete all the other layouts from the menu. + +**Question:** The default terminal does not accept (not even from the clipboard) nor display certain language-specific characters such as umlauts. + +> **Answer:** Using a terminal such as xterm will allow reading and writing special characters. + +**Question:** Users who use high resolutions on small displays and have set their host machines DPI manually, for example through .Xresources on Linux (X11), may find that everything is too small to be read efficiently. (Also helpful to users who have difficulties in reading the fonts and other visual information on the image due to the size of the graphical components.) + +> **Answer:** The DPI can easily be adjusted from Xfce menu → Preferences → Appearance → Fonts → DPI. This enhances the readability and general usability significantly. + +**Question:** Resizing the VM window doesn't resize its contents. + +> **Answer:** This appears to only occur when a new VM image is launched for the first time. The contents should resize after several minutes (up to half an hour), and the problem should not manifest when the VM image is opened a second time. + + + +[installVB]: +[installVB2]: +[cmsvmimagecc7]: +[getstartedcms]: diff --git a/cernopendata/modules/fixtures/data/records/atlas-CERN-EP-2023-174.json b/cernopendata/modules/fixtures/data/records/atlas-CERN-EP-2023-174.json new file mode 100644 index 0000000000..0aba5828cf --- /dev/null +++ b/cernopendata/modules/fixtures/data/records/atlas-CERN-EP-2023-174.json @@ -0,0 +1,242 @@ +[ + { + "abstract": { + "description": "

For this new study, researchers looked for charginos decaying in three ways – via two W bosons (WW), a W boson and a Z boson (WZ), or a W boson and a Higgs boson (WH). These decay channels can all result in similar experimental signatures with one lepton. Researchers looked for unique collision-event signatures with isolated leptons, missing momentum, and large-radius jets (or b-jets in the WH case). They applied improved cut-and-count strategies in the WW/WZ cases, and revised the previous cut-and-count WH analysis with new machine-learning techniques. Using Boosted Decision Trees (BDTs), researchers were able to enhance signal identification in scenarios where the chargino and next-to-lightest neutralino decays were mediated by a Higgs boson, or when their mass difference closely aligns with the mass of the Higgs boson itself.

Researchers utilised this open dataset for training the analysis BDTs, making it readily available for subsequent advanced theoretical or machine learning investigations. The dataset is organised into 16 folders, each containing root files derived from Monte Carlo (MC) simulations. These files encompass both object-level and event-level variables, incorporating their associated systematic uncertainties.

Within these folders, 14 pertain to Standard Model background samples, with three major contributors being Single Top, ttbar, and W jets. The remaining two folders house signal samples and theory uncertainties for all MC-generated events. Each file is enriched with additional variables representing BDT scores for both Signal and Backgrounds.

Adopting a 1 vs all strategy, separate BDTs undergo individual training, reweighing, and optimisation tailored to specific classifications. The resultant scores conform to a comprehensive classification framework, providing sample-targeted independent probabilities spanning from 0 to 1 for all noteworthy Backgrounds and Signal categories. These scores serve as benchmarks for evaluating other cutting-edge models, such as Graph Neural Networks (GNNs), in the ongoing exploration of competitive state-of-the-art methodologies.

The dataset contains a total number of 12,380,322 events of which more than 6 million are ttbar events, 463,056 events in MC-generated Signal samples, and 23,251,217 events in theory samples.

" + }, + "accelerator": "CERN-LHC", + "collaboration": { + "name": "ATLAS collaboration" + }, + "collections": [ + "ATLAS-Derived-Datasets" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "root" + ], + "number_events": 36094595, + "number_files": 1076, + "size": 618957496181 + }, + "doi": "10.7483/OPENDATA.ATLAS.KG0B.XX5J", + "experiment": [ + "ATLAS" + ], + "files": [ + { + "checksum": "adler32:6ca3481a", + "size": 17653, + "type": "index.json", + "uri": "root://eospublic.cern.ch//eos/opendata/atlas/datascience/CERN-EP-2023-174/Wh_24_01_28/file-indexes/Wh_24_01_28_Higgs_samples_root_file_index.json" + }, + { + "checksum": "adler32:70626c5b", + "size": 8833, + "type": "index.txt", + "uri": "root://eospublic.cern.ch//eos/opendata/atlas/datascience/CERN-EP-2023-174/Wh_24_01_28/file-indexes/Wh_24_01_28_Higgs_samples_root_file_index.txt" + }, + { + "checksum": "adler32:14985e68", + "size": 219747, + "type": "index.json", + "uri": 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0000000000..fd8ca2e1fb --- /dev/null +++ b/cernopendata/modules/fixtures/data/records/cms-derived-nanoaodrun1.json @@ -0,0 +1,2790 @@ +[ + { + "abstract": { + "description": "

DYJetsToLL_M-50_7TeV-madgraph-pythia6-tauola dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. MonteCarlo11_Summer11LegDR_DYJetsToLL_M-50_7TeV-madgraph-pythia6-tauola_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31100/MonteCarlo11_Summer11LegDR_DYJetsToLL_M-50_7TeV-madgraph-pythia6-tauola_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31100/MonteCarlo11_Summer11LegDR_DYJetsToLL_M-50_7TeV-madgraph-pythia6-tauola_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-run1", + "root" + ], + "number_events": 34926233, + "number_files": 188, + "size": 97825100 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31100", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "1394", + "type": "isChildOf" + } + ], + "title": "DYJetsToLL_M-50_7TeV-madgraph-pythia6-tauola dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

TTTo2L2Nu2B_7TeV-powheg-pythia6 dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. MonteCarlo11_Summer11LegDR_TTTo2L2Nu2B_7TeV-powheg-pythia6_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31101/MonteCarlo11_Summer11LegDR_TTTo2L2Nu2B_7TeV-powheg-pythia6_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31101/MonteCarlo11_Summer11LegDR_TTTo2L2Nu2B_7TeV-powheg-pythia6_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-run1", + "root" + ], + "number_events": 9771205, + "number_files": 17, + "size": 49740759 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31101", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "1360", + "type": "isChildOf" + } + ], + "title": "TTTo2L2Nu2B_7TeV-powheg-pythia6 dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

TTbar_8TeV-Madspin_aMCatNLO-herwig dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. MonteCarlo12_Summer12_DR53X_TTbar_8TeV-Madspin_aMCatNLO-herwig_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31102/MonteCarlo12_Summer12_DR53X_TTbar_8TeV-Madspin_aMCatNLO-herwig_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31102/MonteCarlo12_Summer12_DR53X_TTbar_8TeV-Madspin_aMCatNLO-herwig_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-run1", + "root" + ], + "number_events": 6423106, + "number_files": 18, + "size": 30978175 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31102", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "9518", + "type": "isChildOf" + } + ], + "title": "TTbar_8TeV-Madspin_aMCatNLO-herwig dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2010A_EG dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2010A_EG_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31103/Run2010A_EG_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31103/Run2010A_EG_doc.html" + }, + "date_created": [ + "2010" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 47187984, + "number_files": 88, + "size": 29466084 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31103", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "83", + "type": "isChildOf" + } + ], + "title": "Run2010A_EG dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2010A_Mu dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2010A_Mu_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31104/Run2010A_Mu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31104/Run2010A_Mu_doc.html" + }, + "date_created": [ + "2010" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 20850125, + "number_files": 40, + "size": 13460112 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31104", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "77", + "type": "isChildOf" + } + ], + "title": "Run2010A_Mu dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2010A_MuOnia dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2010A_MuOnia_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31105/Run2010A_MuOnia_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31105/Run2010A_MuOnia_doc.html" + }, + "date_created": [ + "2010" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 29583697, + "number_files": 65, + "size": 21183852 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31105", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "75", + "type": "isChildOf" + } + ], + "title": "Run2010A_MuOnia dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2010B_Electron dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2010B_Electron_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31106/Run2010B_Electron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31106/Run2010B_Electron_doc.html" + }, + "date_created": [ + "2010" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 27856626, + "number_files": 81, + "size": 24110900 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31106", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "4", + "type": "isChildOf" + } + ], + "title": "Run2010B_Electron dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2010B_Jet dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2010B_Jet_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31107/Run2010B_Jet_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31107/Run2010B_Jet_doc.html" + }, + "date_created": [ + "2010" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 16341187, + "number_files": 42, + "size": 12596211 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31107", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "5", + "type": "isChildOf" + } + ], + "title": "Run2010B_Jet dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2010B_Mu dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2010B_Mu_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31108/Run2010B_Mu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31108/Run2010B_Mu_doc.html" + }, + "date_created": [ + "2010" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 26718043, + "number_files": 75, + "size": 26723593 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31108", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "14", + "type": "isChildOf" + } + ], + "title": "Run2010B_Mu dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2010B_MuOnia dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2010B_MuOnia_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31109/Run2010B_MuOnia_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31109/Run2010B_MuOnia_doc.html" + }, + "date_created": [ + "2010" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 22677534, + "number_files": 73, + "size": 24284679 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31109", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "10", + "type": "isChildOf" + } + ], + "title": "Run2010B_MuOnia dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011A_DoubleElectron dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011A_DoubleElectron_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31110/Run2011A_DoubleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31110/Run2011A_DoubleElectron_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 44239644, + "number_files": 43, + "size": 64547332 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31110", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "16", + "type": "isChildOf" + } + ], + "title": "Run2011A_DoubleElectron dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011A_DoubleMu dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011A_DoubleMu_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31111/Run2011A_DoubleMu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31111/Run2011A_DoubleMu_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 35287778, + "number_files": 35, + "size": 52140430 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31111", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "17", + "type": "isChildOf" + } + ], + "title": "Run2011A_DoubleMu dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011A_Jet dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011A_Jet_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31112/Run2011A_Jet_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31112/Run2011A_Jet_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 26277742, + "number_files": 31, + "size": 52902894 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31112", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "21", + "type": "isChildOf" + } + ], + "title": "Run2011A_Jet dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011A_MuOnia dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011A_MuOnia_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31113/Run2011A_MuOnia_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31113/Run2011A_MuOnia_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 55915322, + "number_files": 58, + "size": 79626551 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31113", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "27", + "type": "isChildOf" + } + ], + "title": "Run2011A_MuOnia dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011A_SingleElectron dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011A_SingleElectron_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31114/Run2011A_SingleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31114/Run2011A_SingleElectron_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 37917536, + "number_files": 39, + "size": 67852776 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31114", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "31", + "type": "isChildOf" + } + ], + "title": "Run2011A_SingleElectron dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011A_SingleMu dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011A_SingleMu_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31115/Run2011A_SingleMu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31115/Run2011A_SingleMu_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 78757263, + "number_files": 100, + "size": 121509784 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31115", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "32", + "type": "isChildOf" + } + ], + "title": "Run2011A_SingleMu dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011B_DoubleElectron dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011B_DoubleElectron_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31116/Run2011B_DoubleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31116/Run2011B_DoubleElectron_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 14588696, + "number_files": 25, + "size": 35748992 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31116", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "271", + "type": "isChildOf" + } + ], + "title": "Run2011B_DoubleElectron dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011B_DoubleMu dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011B_DoubleMu_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31117/Run2011B_DoubleMu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31117/Run2011B_DoubleMu_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 22334391, + "number_files": 35, + "size": 48506867 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31117", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "272", + "type": "isChildOf" + } + ], + "title": "Run2011B_DoubleMu dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011B_Jet dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011B_Jet_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31118/Run2011B_Jet_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31118/Run2011B_Jet_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 12069498, + "number_files": 21, + "size": 38545896 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31118", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "275", + "type": "isChildOf" + } + ], + "title": "Run2011B_Jet dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011B_MuOnia dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011B_MuOnia_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31119/Run2011B_MuOnia_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31119/Run2011B_MuOnia_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 26280382, + "number_files": 39, + "size": 52354586 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31119", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "280", + "type": "isChildOf" + } + ], + "title": "Run2011B_MuOnia dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011B_SingleElectron dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011B_SingleElectron_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31120/Run2011B_SingleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31120/Run2011B_SingleElectron_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 15956053, + "number_files": 25, + "size": 49131393 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31120", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "284", + "type": "isChildOf" + } + ], + "title": "Run2011B_SingleElectron dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2011B_SingleMu dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2011B_SingleMu_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "7TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31121/Run2011B_SingleMu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31121/Run2011B_SingleMu_doc.html" + }, + "date_created": [ + "2011" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 47134514, + "number_files": 93, + "size": 135693716 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31121", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "285", + "type": "isChildOf" + } + ], + "title": "Run2011B_SingleMu dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012B_DoubleElectron dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012B_DoubleElectron_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31122/Run2012B_DoubleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31122/Run2012B_DoubleElectron_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 21474287, + "number_files": 42, + "size": 53390189 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31122", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6003", + "type": "isChildOf" + } + ], + "title": "Run2012B_DoubleElectron dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012B_DoubleMuParked dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012B_DoubleMuParked_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31123/Run2012B_DoubleMuParked_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31123/Run2012B_DoubleMuParked_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 26084708, + "number_files": 57, + "size": 79256573 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31123", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6004", + "type": "isChildOf" + } + ], + "title": "Run2012B_DoubleMuParked dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012B_MuOnia dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012B_MuOnia_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31124/Run2012B_MuOnia_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31124/Run2012B_MuOnia_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 34025601, + "number_files": 64, + "size": 90182715 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31124", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6016", + "type": "isChildOf" + } + ], + "title": "Run2012B_MuOnia dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012B_MuOniaParked dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012B_MuOniaParked_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31125/Run2012B_MuOniaParked_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31125/Run2012B_MuOniaParked_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 54116119, + "number_files": 110, + "size": 139545513 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31125", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6017", + "type": "isChildOf" + } + ], + "title": "Run2012B_MuOniaParked dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012B_SingleElectron dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012B_SingleElectron_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31126/Run2012B_SingleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31126/Run2012B_SingleElectron_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 62023592, + "number_files": 133, + "size": 152143352 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31126", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6020", + "type": "isChildOf" + } + ], + "title": "Run2012B_SingleElectron dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012B_SingleMu dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012B_SingleMu_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31127/Run2012B_SingleMu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31127/Run2012B_SingleMu_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 53446198, + "number_files": 107, + "size": 133394178 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31127", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6021", + "type": "isChildOf" + } + ], + "title": "Run2012B_SingleMu dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012C_DoubleElectron dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012C_DoubleElectron_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31128/Run2012C_DoubleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31128/Run2012C_DoubleElectron_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 32537541, + "number_files": 60, + "size": 82257438 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31128", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6029", + "type": "isChildOf" + } + ], + "title": "Run2012C_DoubleElectron dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012C_DoubleMuParked dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012C_DoubleMuParked_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31129/Run2012C_DoubleMuParked_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31129/Run2012C_DoubleMuParked_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 35455705, + "number_files": 74, + "size": 105982515 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31129", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6030", + "type": "isChildOf" + } + ], + "title": "Run2012C_DoubleMuParked dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012C_MuOnia dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012C_MuOnia_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31130/Run2012C_MuOnia_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31130/Run2012C_MuOnia_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 60197132, + "number_files": 110, + "size": 162710217 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31130", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6042", + "type": "isChildOf" + } + ], + "title": "Run2012C_MuOnia dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012C_MuOniaParked dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012C_MuOniaParked_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31131/Run2012C_MuOniaParked_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31131/Run2012C_MuOniaParked_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 126105289, + "number_files": 243, + "size": 326477179 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31131", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6043", + "type": "isChildOf" + } + ], + "title": "Run2012C_MuOniaParked dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012C_SingleElectron dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012C_SingleElectron_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31132/Run2012C_SingleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31132/Run2012C_SingleElectron_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 98626059, + "number_files": 194, + "size": 242416816 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31132", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6046", + "type": "isChildOf" + } + ], + "title": "Run2012C_SingleElectron dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + }, + { + "abstract": { + "description": "

Run2012C_SingleMu dataset in a NanoAOD-like research-level Ntuple format for CMS Run1 data, readable with bare ROOT or other ROOT-compatible software, and containing the per-event information that is needed in most generic analyses. In contrast to the CMS NanoAOD which is derived from MiniAOD, this dataset is processed directly from the AOD format with code provided by the CMS open data group. Not all variables are available. Nevertheless, there is a large overlap in functionality and content between this format and the standard NanoAOD such that common analyses are possible.

The dataset is provided as a collection of root files. Run2012C_SingleMu_merged.root contains the separate files merged into one file. This dataset was processsed from the primary dataset in AOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "8TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31133/Run2012C_SingleMu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/NanoAODRun1/31133/Run2012C_SingleMu_doc.html" + }, + "date_created": [ + "2012" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-run1", + "root" + ], + "number_events": 85731835, + "number_files": 157, + "size": 215970803 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12505" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31133", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "6047", + "type": "isChildOf" + } + ], + "title": "Run2012C_SingleMu dataset in Run1 NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs.

\n" + } + } +] diff --git a/cernopendata/modules/fixtures/data/records/cms-derived-pfnano-2016.json b/cernopendata/modules/fixtures/data/records/cms-derived-pfnano-2016.json new file mode 100644 index 0000000000..e0c9071e71 --- /dev/null +++ b/cernopendata/modules/fixtures/data/records/cms-derived-pfnano-2016.json @@ -0,0 +1,1542 @@ +[ + { + "abstract": { + "description": "

BTagCSV dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31300/BTagCSV_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31300/BTagCSV_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 100826567, + "number_files": 468, + "size": 1297795768 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31300", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30500", + "type": "isChildOf" + } + ], + "title": "BTagCSV dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

BTagMu dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31301/BTagMu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31301/BTagMu_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 27536603, + "number_files": 91, + "size": 320657946 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31301", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30501", + "type": "isChildOf" + } + ], + "title": "BTagMu dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

Charmonium dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31302/Charmonium_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31302/Charmonium_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 62080523, + "number_files": 205, + "size": 673570329 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31302", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30502", + "type": "isChildOf" + } + ], + "title": "Charmonium dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

DisplacedJet dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31303/DisplacedJet_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31303/DisplacedJet_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 18289323, + "number_files": 79, + "size": 225286816 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31303", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30503", + "type": "isChildOf" + } + ], + "title": "DisplacedJet dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

DoubleEG dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31304/DoubleEG_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31304/DoubleEG_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 78216635, + "number_files": 355, + "size": 893878988 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31304", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30504", + "type": "isChildOf" + } + ], + "title": "DoubleEG dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n", + "links": [ + { + "url": "link to processedLumis.json" + } + ] + } + }, + { + "abstract": { + "description": "

DoubleMuon dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31305/DoubleMuon_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31305/DoubleMuon_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 45235604, + "number_files": 151, + "size": 529653350 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31305", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30505", + "type": "isChildOf" + } + ], + "title": "DoubleMuon dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

DoubleMuonLowMass dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31306/DoubleMuonLowMass_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31306/DoubleMuonLowMass_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 45367551, + "number_files": 133, + "size": 498873700 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31306", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30506", + "type": "isChildOf" + } + ], + "title": "DoubleMuonLowMass dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

HTMHT dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31307/HTMHT_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31307/HTMHT_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 32367421, + "number_files": 143, + "size": 402556267 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31307", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30507", + "type": "isChildOf" + } + ], + "title": "HTMHT dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

JetHT dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31308/JetHT_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31308/JetHT_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 120517157, + "number_files": 842, + "size": 1486368460 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31308", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30508", + "type": "isChildOf" + } + ], + "title": "JetHT dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n", + "links": [ + { + "url": "link to processedLumis.json" + } + ] + } + }, + { + "abstract": { + "description": "

MET dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31309/MET_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31309/MET_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 26974131, + "number_files": 109, + "size": 339156181 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31309", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30509", + "type": "isChildOf" + } + ], + "title": "MET dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

MuOnia dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31310/MuOnia_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31310/MuOnia_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 35301548, + "number_files": 127, + "size": 379335688 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31310", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30510", + "type": "isChildOf" + } + ], + "title": "MuOnia dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

MuonEG dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31311/MuonEG_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31311/MuonEG_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 33854612, + "number_files": 119, + "size": 405546762 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31311", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30511", + "type": "isChildOf" + } + ], + "title": "MuonEG dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

SingleElectron dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31312/SingleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31312/SingleElectron_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 153363109, + "number_files": 556, + "size": 1722259073 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31312", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30512", + "type": "isChildOf" + } + ], + "title": "SingleElectron dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

SingleMuon dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31313/SingleMuon_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31313/SingleMuon_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 149916849, + "number_files": 381, + "size": 1658003182 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31313", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30513", + "type": "isChildOf" + } + ], + "title": "SingleMuon dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

SinglePhoton dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31314/SinglePhoton_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31314/SinglePhoton_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 33288854, + "number_files": 122, + "size": 378974160 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31314", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30514", + "type": "isChildOf" + } + ], + "title": "SinglePhoton dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

Tau dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31315/Tau_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31315/Tau_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 79578661, + "number_files": 370, + "size": 922922704 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31315", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30515", + "type": "isChildOf" + } + ], + "title": "Tau dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + }, + { + "abstract": { + "description": "

ZeroBias dataset in NanoAOD format enhanced with Particle Flow candidates, readable with bare ROOT or other ROOT-compatible software. In addition to the default NanoAOD content, it contains candidates from the Particle Flow algorithm. Their properties are available in the \"PFCands\" collection. This dataset was derived from the primary dataset in MiniAOD format linked below.

The list of validated runs, which must be applied to all analyses, either with the full validation or for an analysis requiring only muons, can be found in:

\n", + "links": [ + { + "recid": "14220" + }, + { + "recid": "14221" + } + ] + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31316/ZeroBias_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/derived-data/PFNano/31316/ZeroBias_doc.html" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-pf", + "root" + ], + "number_events": 27123616, + "number_files": 67, + "size": 219858693 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12504" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31316", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "30516", + "type": "isChildOf" + } + ], + "title": "ZeroBias dataset in NanoAOD format enhanced with Particle Flow candidates from RunG of 2016", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "usage": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. See the instructions for getting started in", + "links": [ + { + "description": "Using Docker containers", + "url": "/docs/cms-guide-docker#nanoaod" + }, + { + "description": "Getting started with CMS NanoAOD", + "url": "/docs/cms-getting-started-nanoaod" + } + ] + }, + "validation": { + "description": "

These data were processed from the MiniAOD primary dataset. If not equal to the parent, the processed runs and lumi sections are available below.

\n" + } + } +] diff --git a/cernopendata/modules/fixtures/data/records/cms-derived-poet-2015.json b/cernopendata/modules/fixtures/data/records/cms-derived-poet-2015.json new file mode 100644 index 0000000000..76c457781c --- /dev/null +++ b/cernopendata/modules/fixtures/data/records/cms-derived-poet-2015.json @@ -0,0 +1,4236 @@ +[ + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /SingleElectron/Run2015D-08Jun2016-v1/MINIAOD dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. Run2015D_SingleElectron_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-poet", + "root" + ], + "number_events": 14393070, + "number_files": 149, + "size": 9924117 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31000", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "24120", + "type": "isChildOf" + } + ], + "title": "Run2015D_SingleElectron dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /SingleMuon/Run2015D-16Dec2015-v1/MINIAOD dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. Run2015D_SingleMuon_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaod-poet", + "root" + ], + "number_events": 22225949, + "number_files": 95, + "size": 14313793 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31001", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "24119", + "type": "isChildOf" + } + ], + "title": "Run2015D_SingleMuon dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /BprimeBprime_M-1200_TuneCUETP8M1_13TeV-madgraph-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_BprimeBprime_M-1200_TuneCUETP8M1_13TeV-madgraph-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 198296, + "number_files": 3, + "size": 463774 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31002", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "15852", + "type": "isChildOf" + } + ], + "title": "BprimeBprime_M-1200_TuneCUETP8M1_13TeV-madgraph-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /BprimeBprime_M-700_TuneCUETP8M1_13TeV-madgraph-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_BprimeBprime_M-700_TuneCUETP8M1_13TeV-madgraph-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 201993, + "number_files": 3, + "size": 434456 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31003", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "15859", + "type": "isChildOf" + } + ], + "title": "BprimeBprime_M-700_TuneCUETP8M1_13TeV-madgraph-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /BprimeBprime_M-800_TuneCUETP8M1_13TeV-madgraph-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_BprimeBprime_M-800_TuneCUETP8M1_13TeV-madgraph-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 203827, + "number_files": 3, + "size": 448250 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31004", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "15860", + "type": "isChildOf" + } + ], + "title": "BprimeBprime_M-800_TuneCUETP8M1_13TeV-madgraph-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /DYJetsToLL_M-50_HT-100to200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_DYJetsToLL_M-50_HT-100to200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 1171208, + "number_files": 3, + "size": 1311889 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31005", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "16443", + "type": "isChildOf" + } + ], + "title": "DYJetsToLL_M-50_HT-100to200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /DYJetsToLL_M-50_HT-200to400_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_DYJetsToLL_M-50_HT-200to400_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 450599, + "number_files": 3, + "size": 591518 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31006", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "16446", + "type": "isChildOf" + } + ], + "title": "DYJetsToLL_M-50_HT-200to400_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /DYJetsToLL_M-50_HT-400to600_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_DYJetsToLL_M-50_HT-400to600_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 531792, + "number_files": 3, + "size": 834204 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31007", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "16449", + "type": "isChildOf" + } + ], + "title": "DYJetsToLL_M-50_HT-400to600_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /DYJetsToLL_M-50_HT-600toInf_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_DYJetsToLL_M-50_HT-600toInf_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 532082, + "number_files": 3, + "size": 958452 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31008", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "16452", + "type": "isChildOf" + } + ], + "title": "DYJetsToLL_M-50_HT-600toInf_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_HT1000to1500_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_HT1000to1500_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 1854, + "number_files": 7, + "size": 4076 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31009", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18289", + "type": "isChildOf" + } + ], + "title": "QCD_HT1000to1500_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_HT100to200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_HT100to200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 2362, + "number_files": 97, + "size": 12304 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31010", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18292", + "type": "isChildOf" + } + ], + "title": "QCD_HT100to200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_HT1500to2000_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_HT1500to2000_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 1783, + "number_files": 5, + "size": 4046 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31011", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18295", + "type": "isChildOf" + } + ], + "title": "QCD_HT1500to2000_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_HT2000toInf_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_HT2000toInf_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 1016, + "number_files": 3, + "size": 2451 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31012", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18299", + "type": "isChildOf" + } + ], + "title": "QCD_HT2000toInf_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_HT200to300_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_HT200to300_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 1469, + "number_files": 23, + "size": 3924 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31013", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18302", + "type": "isChildOf" + } + ], + "title": "QCD_HT200to300_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_HT300to500_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_HT300to500_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 2083, + "number_files": 25, + "size": 5158 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31014", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18306", + "type": "isChildOf" + } + ], + "title": "QCD_HT300to500_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_HT500to700_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_HT500to700_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 3818, + "number_files": 23, + "size": 8096 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31015", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18310", + "type": "isChildOf" + } + ], + "title": "QCD_HT500to700_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_HT700to1000_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_HT700to1000_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 4016, + "number_files": 17, + "size": 8473 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31016", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18314", + "type": "isChildOf" + } + ], + "title": "QCD_HT700to1000_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-1000toInf_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v3/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-1000toInf_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 5776, + "number_files": 3, + "size": 13218 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31017", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18316", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-1000toInf_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-120to170_EMEnriched_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-120to170_EMEnriched_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 9651, + "number_files": 45, + "size": 16473 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31018", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18322", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-120to170_EMEnriched_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-120to170_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-120to170_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 12791, + "number_files": 9, + "size": 17225 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31019", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18323", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-120to170_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-170to300_EMEnriched_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-170to300_EMEnriched_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 5076, + "number_files": 13, + "size": 8457 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31020", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18330", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-170to300_EMEnriched_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-170to300_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-170to300_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 13677, + "number_files": 9, + "size": 21253 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31021", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18331", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-170to300_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-300to470_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-300to470_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 16133, + "number_files": 9, + "size": 29108 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31022", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18335", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-300to470_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-300toInf_EMEnriched_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-300toInf_EMEnriched_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 6683, + "number_files": 9, + "size": 11992 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31023", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18336", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-300toInf_EMEnriched_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-470to600_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-470to600_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 8991, + "number_files": 5, + "size": 17630 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31024", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18348", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-470to600_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-600to800_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v3/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-600to800_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 5226, + "number_files": 3, + "size": 10764 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31025", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18351", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-600to800_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-800to1000_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-800to1000_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 5259, + "number_files": 3, + "size": 11402 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31026", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18352", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-800to1000_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-80to120_EMEnriched_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-80to120_EMEnriched_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 6238, + "number_files": 43, + "size": 11318 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31027", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18353", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-80to120_EMEnriched_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt-80to120_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt-80to120_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 21711, + "number_files": 17, + "size": 26756 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31028", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18354", + "type": "isChildOf" + } + ], + "title": "QCD_Pt-80to120_MuEnrichedPt5_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt_170to250_bcToE_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt_170to250_bcToE_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 5219, + "number_files": 11, + "size": 8439 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31029", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18362", + "type": "isChildOf" + } + ], + "title": "QCD_Pt_170to250_bcToE_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt_250toInf_bcToE_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt_250toInf_bcToE_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 7522, + "number_files": 15, + "size": 13854 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31030", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18367", + "type": "isChildOf" + } + ], + "title": "QCD_Pt_250toInf_bcToE_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /QCD_Pt_80to170_bcToE_TuneCUETP8M1_13TeV_pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_QCD_Pt_80to170_bcToE_TuneCUETP8M1_13TeV_pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 7092, + "number_files": 17, + "size": 9846 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31031", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "18379", + "type": "isChildOf" + } + ], + "title": "QCD_Pt_80to170_bcToE_TuneCUETP8M1_13TeV_pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /ST_s-channel_4f_leptonDecays_13TeV-amcatnlo-pythia8_TuneCUETP8M1/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v2/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_ST_s-channel_4f_leptonDecays_13TeV-amcatnlo-pythia8_TuneCUETP8M1_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 270793, + "number_files": 3, + "size": 294658 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31032", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19395", + "type": "isChildOf" + } + ], + "title": "ST_s-channel_4f_leptonDecays_13TeV-amcatnlo-pythia8_TuneCUETP8M1 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /ST_t-channel_4f_leptonDecays_13TeV-amcatnlo-pythia8_TuneCUETP8M1/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_ST_t-channel_4f_leptonDecays_13TeV-amcatnlo-pythia8_TuneCUETP8M1_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 6025474, + "number_files": 23, + "size": 6465597 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31033", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19397", + "type": "isChildOf" + } + ], + "title": "ST_t-channel_4f_leptonDecays_13TeV-amcatnlo-pythia8_TuneCUETP8M1 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /ST_t-channel_antitop_4f_leptonDecays_13TeV-powheg-pythia8_TuneCUETP8M1/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_ST_t-channel_antitop_4f_leptonDecays_13TeV-powheg-pythia8_TuneCUETP8M1_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 526114, + "number_files": 3, + "size": 563098 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31034", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19407", + "type": "isChildOf" + } + ], + "title": "ST_t-channel_antitop_4f_leptonDecays_13TeV-powheg-pythia8_TuneCUETP8M1 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /ST_tW_antitop_5f_inclusiveDecays_13TeV-powheg-pythia8_TuneCUETP8M1/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_ST_tW_antitop_5f_inclusiveDecays_13TeV-powheg-pythia8_TuneCUETP8M1_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 225319, + "number_files": 3, + "size": 277378 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31035", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19412", + "type": "isChildOf" + } + ], + "title": "ST_tW_antitop_5f_inclusiveDecays_13TeV-powheg-pythia8_TuneCUETP8M1 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /ST_tW_top_5f_inclusiveDecays_13TeV-powheg-pythia8_TuneCUETP8M1/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_ST_tW_top_5f_inclusiveDecays_13TeV-powheg-pythia8_TuneCUETP8M1_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 225039, + "number_files": 3, + "size": 277167 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31036", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19419", + "type": "isChildOf" + } + ], + "title": "ST_tW_top_5f_inclusiveDecays_13TeV-powheg-pythia8_TuneCUETP8M1 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /TTJets_TuneCUETP8M1_13TeV-amcatnloFXFX-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_TTJets_TuneCUETP8M1_13TeV-amcatnloFXFX-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 8226395, + "number_files": 45, + "size": 11793011 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31037", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19949", + "type": "isChildOf" + } + ], + "title": "TTJets_TuneCUETP8M1_13TeV-amcatnloFXFX-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /TT_Mtt-1000toInf_TuneCUETP8M1_13TeV-powheg-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12_ext2-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_TT_Mtt-1000toInf_TuneCUETP8M1_13TeV-powheg-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 5271919, + "number_files": 29, + "size": 8225952 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31038", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19974", + "type": "isChildOf" + } + ], + "title": "TT_Mtt-1000toInf_TuneCUETP8M1_13TeV-powheg-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /TT_Mtt-700to1000_TuneCUETP8M1_13TeV-powheg-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_TT_Mtt-700to1000_TuneCUETP8M1_13TeV-powheg-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 8333982, + "number_files": 51, + "size": 12293712 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31039", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19975", + "type": "isChildOf" + } + ], + "title": "TT_Mtt-700to1000_TuneCUETP8M1_13TeV-powheg-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /TT_TuneCUETP8M1_13TeV-powheg-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12_ext3-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_TT_TuneCUETP8M1_13TeV-powheg-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 20620375, + "number_files": 121, + "size": 28101387 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31040", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19980", + "type": "isChildOf" + } + ], + "title": "TT_TuneCUETP8M1_13TeV-powheg-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /TT_TuneCUETP8M1_13TeV-powheg-scaledown-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12_ext3-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_TT_TuneCUETP8M1_13TeV-powheg-scaledown-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 8180071, + "number_files": 45, + "size": 11135053 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31041", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19983", + "type": "isChildOf" + } + ], + "title": "TT_TuneCUETP8M1_13TeV-powheg-scaledown-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /TT_TuneCUETP8M1_13TeV-powheg-scaleup-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12_ext3-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_TT_TuneCUETP8M1_13TeV-powheg-scaleup-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 8178182, + "number_files": 45, + "size": 11130476 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31042", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19985", + "type": "isChildOf" + } + ], + "title": "TT_TuneCUETP8M1_13TeV-powheg-scaleup-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /TT_TuneEE5C_13TeV-powheg-herwigpp/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_TT_TuneEE5C_13TeV-powheg-herwigpp_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 4116127, + "number_files": 23, + "size": 5525957 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31043", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "19999", + "type": "isChildOf" + } + ], + "title": "TT_TuneEE5C_13TeV-powheg-herwigpp dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /TprimeTprime_M-1200_TuneCUETP8M1_13TeV-madgraph-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_TprimeTprime_M-1200_TuneCUETP8M1_13TeV-madgraph-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 253993, + "number_files": 3, + "size": 603851 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31044", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20225", + "type": "isChildOf" + } + ], + "title": "TprimeTprime_M-1200_TuneCUETP8M1_13TeV-madgraph-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /TprimeTprime_M-700_TuneCUETP8M1_13TeV-madgraph-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_TprimeTprime_M-700_TuneCUETP8M1_13TeV-madgraph-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 256942, + "number_files": 3, + "size": 563235 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31045", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20232", + "type": "isChildOf" + } + ], + "title": "TprimeTprime_M-700_TuneCUETP8M1_13TeV-madgraph-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /TprimeTprime_M-800_TuneCUETP8M1_13TeV-madgraph-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_TprimeTprime_M-800_TuneCUETP8M1_13TeV-madgraph-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 252828, + "number_files": 3, + "size": 566858 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31046", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20233", + "type": "isChildOf" + } + ], + "title": "TprimeTprime_M-800_TuneCUETP8M1_13TeV-madgraph-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /WJetsToLNu_HT-100To200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_WJetsToLNu_HT-100To200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 2633561, + "number_files": 13, + "size": 2525395 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31047", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20531", + "type": "isChildOf" + } + ], + "title": "WJetsToLNu_HT-100To200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /WJetsToLNu_HT-1200To2500_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_WJetsToLNu_HT-1200To2500_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 82780, + "number_files": 3, + "size": 156494 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31048", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20533", + "type": "isChildOf" + } + ], + "title": "WJetsToLNu_HT-1200To2500_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /WJetsToLNu_HT-200To400_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_WJetsToLNu_HT-200To400_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 1386027, + "number_files": 7, + "size": 1583995 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31049", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20535", + "type": "isChildOf" + } + ], + "title": "WJetsToLNu_HT-200To400_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /WJetsToLNu_HT-2500ToInf_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_WJetsToLNu_HT-2500ToInf_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 87234, + "number_files": 3, + "size": 195797 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31050", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20537", + "type": "isChildOf" + } + ], + "title": "WJetsToLNu_HT-2500ToInf_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /WJetsToLNu_HT-400To600_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_WJetsToLNu_HT-400To600_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 588679, + "number_files": 3, + "size": 818463 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31051", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20539", + "type": "isChildOf" + } + ], + "title": "WJetsToLNu_HT-400To600_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /WJetsToLNu_HT-600To800_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_WJetsToLNu_HT-600To800_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 1195542, + "number_files": 5, + "size": 1861935 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31052", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20541", + "type": "isChildOf" + } + ], + "title": "WJetsToLNu_HT-600To800_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /WJetsToLNu_HT-800To1200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_WJetsToLNu_HT-800To1200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 512924, + "number_files": 3, + "size": 868184 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31053", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20544", + "type": "isChildOf" + } + ], + "title": "WJetsToLNu_HT-800To1200_TuneCUETP8M1_13TeV-madgraphMLM-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /WJetsToLNu_TuneCUETP8M1_13TeV-amcatnloFXFX-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12_ext4-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_WJetsToLNu_TuneCUETP8M1_13TeV-amcatnloFXFX-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 38597998, + "number_files": 229, + "size": 29796842 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31054", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20548", + "type": "isChildOf" + } + ], + "title": "WJetsToLNu_TuneCUETP8M1_13TeV-amcatnloFXFX-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /WW_TuneCUETP8M1_13TeV-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_WW_TuneCUETP8M1_13TeV-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 162205, + "number_files": 3, + "size": 155473 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31055", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20677", + "type": "isChildOf" + } + ], + "title": "WW_TuneCUETP8M1_13TeV-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /WZ_TuneCUETP8M1_13TeV-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_WZ_TuneCUETP8M1_13TeV-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 128477, + "number_files": 3, + "size": 130079 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31056", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "20690", + "type": "isChildOf" + } + ], + "title": "WZ_TuneCUETP8M1_13TeV-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + }, + { + "abstract": { + "description": "

This dataset contains information extracted from different physics objects from the 2015 /ZZ_TuneCUETP8M1_13TeV-pythia8/RunIIFall15MiniAODv2-PU25nsData2015v1_76X_mcRun2_asymptotic_v12-v1/MINIAODSIM dataset, readable with bare ROOT or other ROOT-compatible software. It is part of the datasets produced for the CMS open data workshop tutorials, and not all events in the parent dataset were necessarily processed.

It is provided in two different structures: a collection of root files as a direct output of POET (separate trees for each object), and \"_flat.root\" files \"flattened\" to a single tree, as required when used in columnar analysis with e.g. awkward array and uproot. RunIIFall15MiniAODv2_ZZ_TuneCUETP8M1_13TeV-pythia8_flat.root has the separate \"_flat.root\" files merged into one file. This dataset was derived from the primary dataset in MiniAOD format linked below.

\n" + }, + "accelerator": "CERN-LHC", + "authors": [ + { + "name": "CMS Open Data group" + } + ], + "collections": [ + "CMS-Derived-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2015" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "nanoaodsim-poet", + "root" + ], + "number_events": 90219, + "number_files": 3, + "size": 101077 + }, + "experiment": [ + "CMS" + ], + "files": [], + "license": { + "attribution": "CC0" + }, + "methodology": { + "description": "The dataset was produced with the software available in the record linked below.", + "links": [ + { + "recid": "12502" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "31057", + "relations": [ + { + "description": "This dataset was derived from:", + "recid": "21600", + "type": "isChildOf" + } + ], + "title": "ZZ_TuneCUETP8M1_13TeV-pythia8 dataset in reduced NanoAOD-like format", + "type": { + "primary": "Dataset", + "secondary": [ + "Derived" + ] + }, + "use_with": { + "description": "You can access these data through XRootD protocol or direct download, and they can be analysed with common ROOT and Python tools. A tutorial lesson is available in", + "links": [ + { + "url": "https://cms-opendata-workshop.github.io/workshop2022-lesson-ttbarljetsanalysis/" + } + ] + }, + "validation": { + "description": "

These data were processed from the primary dataset using only the validated runs. No further validation was done for the output.

\n" + } + } +] diff --git a/cernopendata/modules/fixtures/data/records/cms-primary-datasets-Run2016.json b/cernopendata/modules/fixtures/data/records/cms-primary-datasets-Run2016.json index 380e041dea..b43c09183a 100644 --- a/cernopendata/modules/fixtures/data/records/cms-primary-datasets-Run2016.json +++ b/cernopendata/modules/fixtures/data/records/cms-primary-datasets-Run2016.json @@ -133,7 +133,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-BTagCSV-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleJet90_Double30_DoubleBTagCSV_p087
HLT_DoubleJet90_Double30_TripleBTagCSV_p087
HLT_DoubleJetsC100_DoubleBTagCSV_p014_DoublePFJetsC100MaxDeta1p6
HLT_DoubleJetsC100_DoubleBTagCSV_p026_DoublePFJetsC160
HLT_DoubleJetsC100_SingleBTagCSV_p014_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p014
HLT_DoubleJetsC100_SingleBTagCSV_p026_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p026
HLT_DoubleJetsC112_DoubleBTagCSV_p014_DoublePFJetsC112MaxDeta1p6
HLT_DoubleJetsC112_DoubleBTagCSV_p026_DoublePFJetsC172
HLT_QuadJet45_DoubleBTagCSV_p087
HLT_QuadJet45_TripleBTagCSV_p087
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq460
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq500
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq200
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq240
HLT_Rsq0p02_MR300_TriPFJet80_60_40_BTagCSV_p063_p20_Mbb60_200
HLT_Rsq0p02_MR300_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR400_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR450_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR500_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR550_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two jets, tagged as b-quark jets with combined secondary vertex.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-BTagCSV-UL2016_MiniAODv2
Output dataset: /BTagCSV/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_BTagCSV
Output dataset: /BTagCSV/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleJet90_Double30_DoubleBTagCSV_p087
HLT_DoubleJet90_Double30_TripleBTagCSV_p087
HLT_DoubleJetsC100_DoubleBTagCSV_p014_DoublePFJetsC100MaxDeta1p6
HLT_DoubleJetsC100_DoubleBTagCSV_p026_DoublePFJetsC160
HLT_DoubleJetsC100_SingleBTagCSV_p014_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p014
HLT_DoubleJetsC100_SingleBTagCSV_p026_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p026
HLT_DoubleJetsC112_DoubleBTagCSV_p014_DoublePFJetsC112MaxDeta1p6
HLT_DoubleJetsC112_DoubleBTagCSV_p026_DoublePFJetsC172
HLT_QuadJet45_DoubleBTagCSV_p087
HLT_QuadJet45_TripleBTagCSV_p087
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq460
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq500
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq200
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq240
HLT_Rsq0p02_MR300_TriPFJet80_60_40_BTagCSV_p063_p20_Mbb60_200
HLT_Rsq0p02_MR300_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR400_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR450_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR500_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR550_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -270,15 +270,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -398,7 +398,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-BTagMu-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_BTagMu_AK8Jet300_Mu5
HLT_BTagMu_DiJet110_Mu5
HLT_BTagMu_DiJet170_Mu5
HLT_BTagMu_DiJet20_Mu5
HLT_BTagMu_DiJet40_Mu5
HLT_BTagMu_DiJet70_Mu5
HLT_BTagMu_Jet300_Mu5

" + "description": "

Events stored in this primary dataset were selected because of the presence of a muon from the b-quark decay, and one or more jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-BTagMu-UL2016_MiniAODv2
Output dataset: /BTagMu/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_BTagMu
Output dataset: /BTagMu/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_BTagMu_AK8Jet300_Mu5
HLT_BTagMu_DiJet110_Mu5
HLT_BTagMu_DiJet170_Mu5
HLT_BTagMu_DiJet20_Mu5
HLT_BTagMu_DiJet40_Mu5
HLT_BTagMu_DiJet70_Mu5
HLT_BTagMu_Jet300_Mu5

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -535,15 +535,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -663,7 +663,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-Charmonium-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Jpsi_Muon
HLT_Dimuon0er16_Jpsi_NoOS_NoVertexing
HLT_Dimuon0er16_Jpsi_NoVertexing
HLT_Dimuon10_Jpsi_Barrel
HLT_Dimuon13_PsiPrime
HLT_Dimuon16_Jpsi
HLT_Dimuon20_Jpsi
HLT_Dimuon6_Jpsi_NoVertexing
HLT_Dimuon8_PsiPrime_Barrel
HLT_DoubleMu4_3_Bs
HLT_DoubleMu4_3_Jpsi_Displaced
HLT_DoubleMu4_JpsiTrk_Displaced
HLT_DoubleMu4_PsiPrimeTrk_Displaced
HLT_Mu7p5_L2Mu2_Jpsi
HLT_Mu7p5_Track2_Jpsi
HLT_Mu7p5_Track3p5_Jpsi
HLT_Mu7p5_Track7_Jpsi
HLT_QuadMuon0_Dimuon0_Jpsi

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons, or a muon and a track with some requirements in the invariant mass for selecting low-mass resonances.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-Charmonium-UL2016_MiniAODv2
Output dataset: /Charmonium/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_Charmonium
Output dataset: /Charmonium/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Jpsi_Muon
HLT_Dimuon0er16_Jpsi_NoOS_NoVertexing
HLT_Dimuon0er16_Jpsi_NoVertexing
HLT_Dimuon10_Jpsi_Barrel
HLT_Dimuon13_PsiPrime
HLT_Dimuon16_Jpsi
HLT_Dimuon20_Jpsi
HLT_Dimuon6_Jpsi_NoVertexing
HLT_Dimuon8_PsiPrime_Barrel
HLT_DoubleMu4_3_Bs
HLT_DoubleMu4_3_Jpsi_Displaced
HLT_DoubleMu4_JpsiTrk_Displaced
HLT_DoubleMu4_PsiPrimeTrk_Displaced
HLT_Mu7p5_L2Mu2_Jpsi
HLT_Mu7p5_Track2_Jpsi
HLT_Mu7p5_Track3p5_Jpsi
HLT_Mu7p5_Track7_Jpsi
HLT_QuadMuon0_Dimuon0_Jpsi

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -799,15 +799,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -941,7 +941,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DisplacedJet-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_HT200_DisplacedDijet40_DisplacedTrack
HLT_HT200
HLT_HT250_DisplacedDijet40_DisplacedTrack
HLT_HT275
HLT_HT325
HLT_HT350_DisplacedDijet40_DisplacedTrack
HLT_HT350_DisplacedDijet40_Inclusive
HLT_HT350_DisplacedDijet80_DisplacedTrack
HLT_HT350_DisplacedDijet80_Tight_DisplacedTrack
HLT_HT400_DisplacedDijet40_Inclusive
HLT_HT425
HLT_HT500_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet80_Inclusive
HLT_HT575
HLT_HT650_DisplacedDijet80_Inclusive
HLT_HT750_DisplacedDijet80_Inclusive
HLT_VBF_DisplacedJet40_DisplacedTrack_2TrackIP2DSig5
HLT_VBF_DisplacedJet40_DisplacedTrack
HLT_VBF_DisplacedJet40_Hadronic_2PromptTrack
HLT_VBF_DisplacedJet40_Hadronic
HLT_VBF_DisplacedJet40_TightID_DisplacedTrack
HLT_VBF_DisplacedJet40_TightID_Hadronic
HLT_VBF_DisplacedJet40_VTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VTightID_Hadronic
HLT_VBF_DisplacedJet40_VVTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VVTightID_Hadronic

" + "description": "

Events stored in this primary dataset were selected because of the presence of one or more displaced jets, or a displaced jet and/or high scalar sum of the jet transverse momenta (HT).

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DisplacedJet-UL2016_MiniAODv2
Output dataset: /DisplacedJet/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_DisplacedJet
Output dataset: /DisplacedJet/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_HT200_DisplacedDijet40_DisplacedTrack
HLT_HT200
HLT_HT250_DisplacedDijet40_DisplacedTrack
HLT_HT275
HLT_HT325
HLT_HT350_DisplacedDijet40_DisplacedTrack
HLT_HT350_DisplacedDijet40_Inclusive
HLT_HT350_DisplacedDijet80_DisplacedTrack
HLT_HT350_DisplacedDijet80_Tight_DisplacedTrack
HLT_HT400_DisplacedDijet40_Inclusive
HLT_HT425
HLT_HT500_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet80_Inclusive
HLT_HT575
HLT_HT650_DisplacedDijet80_Inclusive
HLT_HT750_DisplacedDijet80_Inclusive
HLT_VBF_DisplacedJet40_DisplacedTrack_2TrackIP2DSig5
HLT_VBF_DisplacedJet40_DisplacedTrack
HLT_VBF_DisplacedJet40_Hadronic_2PromptTrack
HLT_VBF_DisplacedJet40_Hadronic
HLT_VBF_DisplacedJet40_TightID_DisplacedTrack
HLT_VBF_DisplacedJet40_TightID_Hadronic
HLT_VBF_DisplacedJet40_VTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VTightID_Hadronic
HLT_VBF_DisplacedJet40_VVTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VVTightID_Hadronic

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -1078,15 +1078,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -1262,7 +1262,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DoubleEG-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Diphoton30EB_18EB_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30PV_18PV_R9Id_AND_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelSeedMatch_Mass70
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_Mass90
HLT_Diphoton30_18_Solid_R9Id_AND_IsoCaloId_AND_HE_R9Id_Mass55
HLT_DoubleEle24_22_eta2p1_WPLoose_Gsf
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL_MW
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL
HLT_DoubleEle33_CaloIdL_MW
HLT_DoubleEle33_CaloIdL
HLT_DoubleEle37_Ele27_CaloIdL_GsfTrkIdVL
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_DoublePhoton60
HLT_DoublePhoton85
HLT_ECALHT800
HLT_Ele10_CaloIdM_TrackIdM_CentralPFJet30_BTagCSV_p13
HLT_Ele12_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele12_CaloIdM_TrackIdM_PFJet30
HLT_Ele16_Ele12_Ele8_CaloIdL_TrackIdL
HLT_Ele17_CaloIdL_GsfTrkIdVL
HLT_Ele17_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Ele17_CaloIdM_TrackIdM_PFJet30
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdM_TrackIdM_PFJet30
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ_L1JetTauSeeded
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele27_HighEta_Ele20_Mass55
HLT_Ele30WP60_Ele8_Mass55
HLT_Ele30WP60_SC4_Mass55
HLT_Ele8_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele8_CaloIdM_TrackIdM_PFJet30
HLT_Photon26_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon16_AND_HE10_R9Id65_Eta2_Mass60
HLT_Photon36_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon22_AND_HE10_R9Id65_Eta2_Mass15
HLT_Photon42_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon25_AND_HE10_R9Id65_Eta2_Mass15

" + "description": "

Events stored in this primary dataset were selected because of the presence of different combinations of energetic photons, electrons and/or jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DoubleEG-UL2016_MiniAODv2
Output dataset: /DoubleEG/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_DoubleEG
Output dataset: /DoubleEG/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Diphoton30EB_18EB_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30PV_18PV_R9Id_AND_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelSeedMatch_Mass70
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_Mass90
HLT_Diphoton30_18_Solid_R9Id_AND_IsoCaloId_AND_HE_R9Id_Mass55
HLT_DoubleEle24_22_eta2p1_WPLoose_Gsf
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL_MW
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL
HLT_DoubleEle33_CaloIdL_MW
HLT_DoubleEle33_CaloIdL
HLT_DoubleEle37_Ele27_CaloIdL_GsfTrkIdVL
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_DoublePhoton60
HLT_DoublePhoton85
HLT_ECALHT800
HLT_Ele10_CaloIdM_TrackIdM_CentralPFJet30_BTagCSV_p13
HLT_Ele12_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele12_CaloIdM_TrackIdM_PFJet30
HLT_Ele16_Ele12_Ele8_CaloIdL_TrackIdL
HLT_Ele17_CaloIdL_GsfTrkIdVL
HLT_Ele17_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Ele17_CaloIdM_TrackIdM_PFJet30
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdM_TrackIdM_PFJet30
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ_L1JetTauSeeded
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele27_HighEta_Ele20_Mass55
HLT_Ele30WP60_Ele8_Mass55
HLT_Ele30WP60_SC4_Mass55
HLT_Ele8_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele8_CaloIdM_TrackIdM_PFJet30
HLT_Photon26_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon16_AND_HE10_R9Id65_Eta2_Mass60
HLT_Photon36_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon22_AND_HE10_R9Id65_Eta2_Mass15
HLT_Photon42_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon25_AND_HE10_R9Id65_Eta2_Mass15

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -1396,15 +1396,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -1538,7 +1538,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DoubleMuon-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu0
HLT_DoubleMu18NoFiltersNoVtx
HLT_DoubleMu23NoFiltersNoVtxDisplaced
HLT_DoubleMu28NoFiltersNoVtxDisplaced
HLT_DoubleMu33NoFiltersNoVtx
HLT_DoubleMu38NoFiltersNoVtx
HLT_DoubleMu8_Mass8_PFHT250
HLT_DoubleMu8_Mass8_PFHT300
HLT_L2DoubleMu23_NoVertex
HLT_L2DoubleMu28_NoVertex_2Cha_Angle2p5_Mass10
HLT_L2DoubleMu38_NoVertex_2Cha_Angle2p5_Mass10
HLT_Mu10_CentralPFJet30_BTagCSV_p13
HLT_Mu17_Mu8_DZ
HLT_Mu17_Mu8_SameSign_DZ
HLT_Mu17_Mu8_SameSign
HLT_Mu17_Mu8
HLT_Mu17_TkMu8_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL
HLT_Mu17
HLT_Mu20_Mu10_DZ
HLT_Mu20_Mu10_SameSign_DZ
HLT_Mu20_Mu10_SameSign
HLT_Mu20_Mu10
HLT_Mu27_TkMu8
HLT_Mu30_TkMu11
HLT_Mu3_PFJet40
HLT_Mu40_TkMu11
HLT_Mu8_TrkIsoVVL
HLT_Mu8
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_TripleMu_12_10_5
HLT_TripleMu_5_3_3_DZ_Mass3p8
HLT_TripleMu_5_3_3
HLT_TrkMu15_DoubleTrkMu5NoFiltersNoVtx
HLT_TrkMu17_DoubleTrkMu8NoFiltersNoVtx

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two energetic muons in the event.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DoubleMuon-UL2016_MiniAODv2
Output dataset: /DoubleMuon/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_DoubleMuon
Output dataset: /DoubleMuon/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu0
HLT_DoubleMu18NoFiltersNoVtx
HLT_DoubleMu23NoFiltersNoVtxDisplaced
HLT_DoubleMu28NoFiltersNoVtxDisplaced
HLT_DoubleMu33NoFiltersNoVtx
HLT_DoubleMu38NoFiltersNoVtx
HLT_DoubleMu8_Mass8_PFHT250
HLT_DoubleMu8_Mass8_PFHT300
HLT_L2DoubleMu23_NoVertex
HLT_L2DoubleMu28_NoVertex_2Cha_Angle2p5_Mass10
HLT_L2DoubleMu38_NoVertex_2Cha_Angle2p5_Mass10
HLT_Mu10_CentralPFJet30_BTagCSV_p13
HLT_Mu17_Mu8_DZ
HLT_Mu17_Mu8_SameSign_DZ
HLT_Mu17_Mu8_SameSign
HLT_Mu17_Mu8
HLT_Mu17_TkMu8_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL
HLT_Mu17
HLT_Mu20_Mu10_DZ
HLT_Mu20_Mu10_SameSign_DZ
HLT_Mu20_Mu10_SameSign
HLT_Mu20_Mu10
HLT_Mu27_TkMu8
HLT_Mu30_TkMu11
HLT_Mu3_PFJet40
HLT_Mu40_TkMu11
HLT_Mu8_TrkIsoVVL
HLT_Mu8
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_TripleMu_12_10_5
HLT_TripleMu_5_3_3_DZ_Mass3p8
HLT_TripleMu_5_3_3
HLT_TrkMu15_DoubleTrkMu5NoFiltersNoVtx
HLT_TrkMu17_DoubleTrkMu8NoFiltersNoVtx

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -1674,15 +1674,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -1816,7 +1816,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DoubleMuonLowMass-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu3_Trk_Tau3mu
HLT_DoubleMu4_LowMassNonResonantTrk_Displaced

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons with low invariant mass.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DoubleMuonLowMass-UL2016_MiniAODv2
Output dataset: /DoubleMuonLowMass/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step ReReco-Run2016G-DoubleMuonLowMass-21Feb2020_UL2016
Output dataset: /DoubleMuonLowMass/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu3_Trk_Tau3mu
HLT_DoubleMu4_LowMassNonResonantTrk_Displaced

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -1952,15 +1952,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -2108,7 +2108,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-HTMHT-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu140
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu80
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p57
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p63
HLT_PFHT200_PFAlphaT0p51
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p55
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p58
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p54
HLT_PFHT300_PFMET100
HLT_PFHT300_PFMET110
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p52
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p51
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p52
HLT_Rsq0p25
HLT_Rsq0p30
HLT_RsqMR240_Rsq0p09_MR200_4jet
HLT_RsqMR240_Rsq0p09_MR200
HLT_RsqMR270_Rsq0p09_MR200_4jet
HLT_RsqMR270_Rsq0p09_MR200

" + "description": "

Events stored in this primary dataset were selected because of the presence of a combination of a high scalar sum of the jet transverse momenta (HT), one or more energetic jets, or high missing transverse energy.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-HTMHT-UL2016_MiniAODv2
Output dataset: /HTMHT/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_HTMHT
Output dataset: /HTMHT/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu140
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu80
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p57
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p63
HLT_PFHT200_PFAlphaT0p51
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p55
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p58
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p54
HLT_PFHT300_PFMET100
HLT_PFHT300_PFMET110
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p52
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p51
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p52
HLT_Rsq0p25
HLT_Rsq0p30
HLT_RsqMR240_Rsq0p09_MR200_4jet
HLT_RsqMR240_Rsq0p09_MR200
HLT_RsqMR270_Rsq0p09_MR200_4jet
HLT_RsqMR270_Rsq0p09_MR200

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -2245,15 +2245,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -2429,7 +2429,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-JetHT-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_AK8DiPFJet250_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet250_200_TrimMass30
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet280_200_TrimMass30
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet300_200_TrimMass30
HLT_AK8PFHT600_TrimR0p1PT0p03Mass50_BTagCSV_p20
HLT_AK8PFHT650_TrimR0p1PT0p03Mass50
HLT_AK8PFHT700_TrimR0p1PT0p03Mass50
HLT_AK8PFHT750_TrimMass50
HLT_AK8PFHT800_TrimMass50
HLT_AK8PFJet140
HLT_AK8PFJet200
HLT_AK8PFJet260
HLT_AK8PFJet320
HLT_AK8PFJet360_TrimMass30
HLT_AK8PFJet400_TrimMass30
HLT_AK8PFJet400
HLT_AK8PFJet40
HLT_AK8PFJet450
HLT_AK8PFJet500
HLT_AK8PFJet60
HLT_AK8PFJet80
HLT_CaloJet500_NoJetID
HLT_DiCentralPFJet170_CFMax0p1
HLT_DiCentralPFJet170
HLT_DiCentralPFJet220_CFMax0p3
HLT_DiCentralPFJet330_CFMax0p5
HLT_DiCentralPFJet430
HLT_DiJetVBFMu_PassThrough
HLT_DiJetVBF_PassThrough
HLT_DiPFJetAve100_HFJEC
HLT_DiPFJetAve140
HLT_DiPFJetAve160_HFJEC
HLT_DiPFJetAve200
HLT_DiPFJetAve220_HFJEC
HLT_DiPFJetAve260
HLT_DiPFJetAve300_HFJEC
HLT_DiPFJetAve320
HLT_DiPFJetAve400
HLT_DiPFJetAve40
HLT_DiPFJetAve500
HLT_DiPFJetAve60_HFJEC
HLT_DiPFJetAve60
HLT_DiPFJetAve80_HFJEC
HLT_DiPFJetAve80
HLT_HT2000
HLT_HT2500
HLT_L1_TripleJet_VBF
HLT_PFHT125
HLT_PFHT200
HLT_PFHT250
HLT_PFHT300
HLT_PFHT350
HLT_PFHT400_SixJet30_DoubleBTagCSV_p056
HLT_PFHT400_SixJet30
HLT_PFHT400
HLT_PFHT450_SixJet40_BTagCSV_p056
HLT_PFHT450_SixJet40
HLT_PFHT475
HLT_PFHT550_4JetPt50
HLT_PFHT600
HLT_PFHT650_4JetPt50
HLT_PFHT650_WideJetMJJ900DEtaJJ1p5
HLT_PFHT650_WideJetMJJ950DEtaJJ1p5
HLT_PFHT650
HLT_PFHT750_4JetPt50
HLT_PFHT750_4JetPt70
HLT_PFHT750_4JetPt80
HLT_PFHT800_4JetPt50
HLT_PFHT800
HLT_PFHT850_4JetPt50
HLT_PFHT900
HLT_PFJet140
HLT_PFJet200
HLT_PFJet260
HLT_PFJet320
HLT_PFJet400
HLT_PFJet40
HLT_PFJet450
HLT_PFJet500
HLT_PFJet60
HLT_PFJet80
HLT_QuadPFJet_VBF
HLT_SingleCentralPFJet170_CFMax0p1

" + "description": "

Events stored in this primary dataset were selected because of the presence of a high scalar sum of the jet transverse momenta (HT), or at least one or two energetic jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-JetHT-UL2016_MiniAODv2
Output dataset: /JetHT/Run2016G-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_JetHT
Output dataset: /JetHT/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_AK8DiPFJet250_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet250_200_TrimMass30
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet280_200_TrimMass30
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet300_200_TrimMass30
HLT_AK8PFHT600_TrimR0p1PT0p03Mass50_BTagCSV_p20
HLT_AK8PFHT650_TrimR0p1PT0p03Mass50
HLT_AK8PFHT700_TrimR0p1PT0p03Mass50
HLT_AK8PFHT750_TrimMass50
HLT_AK8PFHT800_TrimMass50
HLT_AK8PFJet140
HLT_AK8PFJet200
HLT_AK8PFJet260
HLT_AK8PFJet320
HLT_AK8PFJet360_TrimMass30
HLT_AK8PFJet400_TrimMass30
HLT_AK8PFJet400
HLT_AK8PFJet40
HLT_AK8PFJet450
HLT_AK8PFJet500
HLT_AK8PFJet60
HLT_AK8PFJet80
HLT_CaloJet500_NoJetID
HLT_DiCentralPFJet170_CFMax0p1
HLT_DiCentralPFJet170
HLT_DiCentralPFJet220_CFMax0p3
HLT_DiCentralPFJet330_CFMax0p5
HLT_DiCentralPFJet430
HLT_DiJetVBFMu_PassThrough
HLT_DiJetVBF_PassThrough
HLT_DiPFJetAve100_HFJEC
HLT_DiPFJetAve140
HLT_DiPFJetAve160_HFJEC
HLT_DiPFJetAve200
HLT_DiPFJetAve220_HFJEC
HLT_DiPFJetAve260
HLT_DiPFJetAve300_HFJEC
HLT_DiPFJetAve320
HLT_DiPFJetAve400
HLT_DiPFJetAve40
HLT_DiPFJetAve500
HLT_DiPFJetAve60_HFJEC
HLT_DiPFJetAve60
HLT_DiPFJetAve80_HFJEC
HLT_DiPFJetAve80
HLT_HT2000
HLT_HT2500
HLT_L1_TripleJet_VBF
HLT_PFHT125
HLT_PFHT200
HLT_PFHT250
HLT_PFHT300
HLT_PFHT350
HLT_PFHT400_SixJet30_DoubleBTagCSV_p056
HLT_PFHT400_SixJet30
HLT_PFHT400
HLT_PFHT450_SixJet40_BTagCSV_p056
HLT_PFHT450_SixJet40
HLT_PFHT475
HLT_PFHT550_4JetPt50
HLT_PFHT600
HLT_PFHT650_4JetPt50
HLT_PFHT650_WideJetMJJ900DEtaJJ1p5
HLT_PFHT650_WideJetMJJ950DEtaJJ1p5
HLT_PFHT650
HLT_PFHT750_4JetPt50
HLT_PFHT750_4JetPt70
HLT_PFHT750_4JetPt80
HLT_PFHT800_4JetPt50
HLT_PFHT800
HLT_PFHT850_4JetPt50
HLT_PFHT900
HLT_PFJet140
HLT_PFJet200
HLT_PFJet260
HLT_PFJet320
HLT_PFJet400
HLT_PFJet40
HLT_PFJet450
HLT_PFJet500
HLT_PFJet60
HLT_PFJet80
HLT_QuadPFJet_VBF
HLT_SingleCentralPFJet170_CFMax0p1

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -2566,15 +2566,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -2722,7 +2722,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-MET-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight_BTagCSV_p067
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight
HLT_DiCentralPFJet55_PFMET110
HLT_DoubleMu3_PFMET50
HLT_MET200
HLT_MET250
HLT_MET300
HLT_MET600
HLT_MET60_IsoTrk35_Loose
HLT_MET700
HLT_MET75_IsoTrk50
HLT_MET90_IsoTrk50
HLT_MonoCentralPFJet80_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_Mu14er_PFMET100
HLT_Mu3er_PFHT140_PFMET125
HLT_Mu6_PFHT200_PFMET100
HLT_Mu6_PFHT200_PFMET80_BTagCSV_p067
HLT_PFMET100_PFMHT100_IDTight_BeamHaloCleaned
HLT_PFMET100_PFMHT100_IDTight
HLT_PFMET110_PFMHT110_IDTight
HLT_PFMET120_BTagCSV_p067
HLT_PFMET120_Mu5
HLT_PFMET120_PFMHT120_IDTight
HLT_PFMET170_BeamHaloCleaned
HLT_PFMET170_HBHECleaned
HLT_PFMET170_HBHE_BeamHaloCleaned
HLT_PFMET170_JetIdCleaned
HLT_PFMET170_NoiseCleaned
HLT_PFMET170_NotCleaned
HLT_PFMET300
HLT_PFMET400
HLT_PFMET500
HLT_PFMET600
HLT_PFMET90_PFMHT90_IDTight
HLT_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_PFMETTypeOne190_HBHE_BeamHaloCleaned

" + "description": "

Events stored in this primary dataset were selected because of the presence of high missing transverse energy.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-MET-UL2016_MiniAODv2
Output dataset: /MET/Run2016G-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_MET
Output dataset: /MET/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight_BTagCSV_p067
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight
HLT_DiCentralPFJet55_PFMET110
HLT_DoubleMu3_PFMET50
HLT_MET200
HLT_MET250
HLT_MET300
HLT_MET600
HLT_MET60_IsoTrk35_Loose
HLT_MET700
HLT_MET75_IsoTrk50
HLT_MET90_IsoTrk50
HLT_MonoCentralPFJet80_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_Mu14er_PFMET100
HLT_Mu3er_PFHT140_PFMET125
HLT_Mu6_PFHT200_PFMET100
HLT_Mu6_PFHT200_PFMET80_BTagCSV_p067
HLT_PFMET100_PFMHT100_IDTight_BeamHaloCleaned
HLT_PFMET100_PFMHT100_IDTight
HLT_PFMET110_PFMHT110_IDTight
HLT_PFMET120_BTagCSV_p067
HLT_PFMET120_Mu5
HLT_PFMET120_PFMHT120_IDTight
HLT_PFMET170_BeamHaloCleaned
HLT_PFMET170_HBHECleaned
HLT_PFMET170_HBHE_BeamHaloCleaned
HLT_PFMET170_JetIdCleaned
HLT_PFMET170_NoiseCleaned
HLT_PFMET170_NotCleaned
HLT_PFMET300
HLT_PFMET400
HLT_PFMET500
HLT_PFMET600
HLT_PFMET90_PFMHT90_IDTight
HLT_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_PFMETTypeOne190_HBHE_BeamHaloCleaned

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -2859,15 +2859,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -2973,7 +2973,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-MuOnia-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Phi_Barrel
HLT_Dimuon0_Upsilon_Muon
HLT_Dimuon13_Upsilon
HLT_Dimuon8_Upsilon_Barrel
HLT_Mu16_TkMu0_dEta18_Onia
HLT_Mu16_TkMu0_dEta18_Phi
HLT_Mu25_TkMu0_dEta18_Onia
HLT_Mu7p5_L2Mu2_Upsilon
HLT_Mu7p5_Track2_Upsilon
HLT_Mu7p5_Track3p5_Upsilon
HLT_Mu7p5_Track7_Upsilon
HLT_QuadMuon0_Dimuon0_Upsilon

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons in the event requiring only very low energy and some requirements in the invariant mass for selecting low-mass resonances.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-MuOnia-UL2016_MiniAODv2
Output dataset: /MuOnia/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_MuOnia
Output dataset: /MuOnia/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Phi_Barrel
HLT_Dimuon0_Upsilon_Muon
HLT_Dimuon13_Upsilon
HLT_Dimuon8_Upsilon_Barrel
HLT_Mu16_TkMu0_dEta18_Onia
HLT_Mu16_TkMu0_dEta18_Phi
HLT_Mu25_TkMu0_dEta18_Onia
HLT_Mu7p5_L2Mu2_Upsilon
HLT_Mu7p5_Track2_Upsilon
HLT_Mu7p5_Track3p5_Upsilon
HLT_Mu7p5_Track7_Upsilon
HLT_QuadMuon0_Dimuon0_Upsilon

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -3109,15 +3109,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -3223,7 +3223,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-MuonEG-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiMu9_Ele9_CaloIdL_TrackIdL
HLT_Mu12_Photon25_CaloIdL_L1ISO
HLT_Mu12_Photon25_CaloIdL_L1OR
HLT_Mu12_Photon25_CaloIdL
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Mu17_Photon22_CaloIdL_L1ISO
HLT_Mu17_Photon30_CaloIdL_L1ISO
HLT_Mu17_Photon35_CaloIdL_L1ISO
HLT_Mu17_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23NoFiltersNoVtx_Photon23_CaloIdL
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL
HLT_Mu27_Ele37_CaloIdL_GsfTrkIdVL
HLT_Mu28NoFiltersNoVtxDisplaced_Photon28_CaloIdL
HLT_Mu30_Ele30_CaloIdL_GsfTrkIdVL
HLT_Mu33NoFiltersNoVtxDisplaced_Photon33_CaloIdL
HLT_Mu33_Ele33_CaloIdL_GsfTrkIdVL
HLT_Mu37_Ele27_CaloIdL_GsfTrkIdVL
HLT_Mu38NoFiltersNoVtx_Photon38_CaloIdL
HLT_Mu42NoFiltersNoVtx_Photon42_CaloIdL
HLT_Mu8_DiEle12_CaloIdL_TrackIdL
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_Mu8_TrkIsoVVL_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL

" + "description": "

Events stored in this primary dataset were selected because of the presence of one energetic muon and electron or photon.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-MuonEG-UL2016_MiniAODv2
Output dataset: /MuonEG/Run2016G-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_MuonEG
Output dataset: /MuonEG/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiMu9_Ele9_CaloIdL_TrackIdL
HLT_Mu12_Photon25_CaloIdL_L1ISO
HLT_Mu12_Photon25_CaloIdL_L1OR
HLT_Mu12_Photon25_CaloIdL
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Mu17_Photon22_CaloIdL_L1ISO
HLT_Mu17_Photon30_CaloIdL_L1ISO
HLT_Mu17_Photon35_CaloIdL_L1ISO
HLT_Mu17_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23NoFiltersNoVtx_Photon23_CaloIdL
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL
HLT_Mu27_Ele37_CaloIdL_GsfTrkIdVL
HLT_Mu28NoFiltersNoVtxDisplaced_Photon28_CaloIdL
HLT_Mu30_Ele30_CaloIdL_GsfTrkIdVL
HLT_Mu33NoFiltersNoVtxDisplaced_Photon33_CaloIdL
HLT_Mu33_Ele33_CaloIdL_GsfTrkIdVL
HLT_Mu37_Ele27_CaloIdL_GsfTrkIdVL
HLT_Mu38NoFiltersNoVtx_Photon38_CaloIdL
HLT_Mu42NoFiltersNoVtx_Photon42_CaloIdL
HLT_Mu8_DiEle12_CaloIdL_TrackIdL
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_Mu8_TrkIsoVVL_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -3359,15 +3359,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -3515,7 +3515,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-SingleElectron-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Ele105_CaloIdVT_GsfTrkIdT
HLT_Ele115_CaloIdVT_GsfTrkIdT
HLT_Ele145_CaloIdVT_GsfTrkIdT
HLT_Ele15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Ele15_IsoVVVL_PFHT350_PFMET50
HLT_Ele15_IsoVVVL_PFHT350
HLT_Ele15_IsoVVVL_PFHT400_PFMET50
HLT_Ele15_IsoVVVL_PFHT400
HLT_Ele15_IsoVVVL_PFHT600
HLT_Ele200_CaloIdVT_GsfTrkIdT
HLT_Ele20_eta2p1_WPLoose_Gsf_LooseIsoPFTau28
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau29
HLT_Ele22_eta2p1_WPLoose_Gsf
HLT_Ele23_WPLoose_Gsf_WHbbBoost
HLT_Ele23_WPLoose_Gsf
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau30
HLT_Ele24_eta2p1_WPLoose_Gsf
HLT_Ele250_CaloIdVT_GsfTrkIdT
HLT_Ele25_WPTight_Gsf
HLT_Ele25_eta2p1_WPLoose_Gsf
HLT_Ele25_eta2p1_WPTight_Gsf
HLT_Ele27_WPLoose_Gsf_WHbbBoost
HLT_Ele27_WPLoose_Gsf
HLT_Ele27_WPTight_Gsf_L1JetTauSeeded
HLT_Ele27_WPTight_Gsf
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_HT200
HLT_Ele27_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele27_eta2p1_WPLoose_Gsf
HLT_Ele27_eta2p1_WPTight_Gsf
HLT_Ele300_CaloIdVT_GsfTrkIdT
HLT_Ele30_WPTight_Gsf
HLT_Ele30_eta2p1_WPTight_Gsf
HLT_Ele32_WPTight_Gsf
HLT_Ele32_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele32_eta2p1_WPTight_Gsf
HLT_Ele35_CaloIdVT_GsfTrkIdT_PFJet150_PFJet50
HLT_Ele35_WPLoose_Gsf
HLT_Ele36_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele45_CaloIdVT_GsfTrkIdT_PFJet200_PFJet50
HLT_Ele45_WPLoose_Gsf_L1JetTauSeeded
HLT_Ele45_WPLoose_Gsf
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet140
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet165
HLT_Ele50_IsoVVVL_PFHT400

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one high-energy electron, or at least one high-energy electron and one or more jets or tau.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-SingleElectron-UL2016_MiniAODv2
Output dataset: /SingleElectron/Run2016G-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_SingleElectron
Output dataset: /SingleElectron/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Ele105_CaloIdVT_GsfTrkIdT
HLT_Ele115_CaloIdVT_GsfTrkIdT
HLT_Ele145_CaloIdVT_GsfTrkIdT
HLT_Ele15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Ele15_IsoVVVL_PFHT350_PFMET50
HLT_Ele15_IsoVVVL_PFHT350
HLT_Ele15_IsoVVVL_PFHT400_PFMET50
HLT_Ele15_IsoVVVL_PFHT400
HLT_Ele15_IsoVVVL_PFHT600
HLT_Ele200_CaloIdVT_GsfTrkIdT
HLT_Ele20_eta2p1_WPLoose_Gsf_LooseIsoPFTau28
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau29
HLT_Ele22_eta2p1_WPLoose_Gsf
HLT_Ele23_WPLoose_Gsf_WHbbBoost
HLT_Ele23_WPLoose_Gsf
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau30
HLT_Ele24_eta2p1_WPLoose_Gsf
HLT_Ele250_CaloIdVT_GsfTrkIdT
HLT_Ele25_WPTight_Gsf
HLT_Ele25_eta2p1_WPLoose_Gsf
HLT_Ele25_eta2p1_WPTight_Gsf
HLT_Ele27_WPLoose_Gsf_WHbbBoost
HLT_Ele27_WPLoose_Gsf
HLT_Ele27_WPTight_Gsf_L1JetTauSeeded
HLT_Ele27_WPTight_Gsf
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_HT200
HLT_Ele27_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele27_eta2p1_WPLoose_Gsf
HLT_Ele27_eta2p1_WPTight_Gsf
HLT_Ele300_CaloIdVT_GsfTrkIdT
HLT_Ele30_WPTight_Gsf
HLT_Ele30_eta2p1_WPTight_Gsf
HLT_Ele32_WPTight_Gsf
HLT_Ele32_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele32_eta2p1_WPTight_Gsf
HLT_Ele35_CaloIdVT_GsfTrkIdT_PFJet150_PFJet50
HLT_Ele35_WPLoose_Gsf
HLT_Ele36_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele45_CaloIdVT_GsfTrkIdT_PFJet200_PFJet50
HLT_Ele45_WPLoose_Gsf_L1JetTauSeeded
HLT_Ele45_WPLoose_Gsf
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet140
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet165
HLT_Ele50_IsoVVVL_PFHT400

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -3649,15 +3649,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -3805,7 +3805,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-SingleMuon-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleIsoMu17_eta2p1_noDzCut
HLT_DoubleIsoMu17_eta2p1
HLT_IsoMu16_eta2p1_MET30_LooseIsoPFTau50_Trk30_eta2p1
HLT_IsoMu16_eta2p1_MET30
HLT_IsoMu17_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu17_eta2p1_LooseIsoPFTau20
HLT_IsoMu18
HLT_IsoMu19_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu19_eta2p1_LooseIsoPFTau20
HLT_IsoMu19_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu20
HLT_IsoMu21_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu21_eta2p1_LooseIsoPFTau50_Trk30_eta2p1_SingleL1
HLT_IsoMu21_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu22_eta2p1
HLT_IsoMu22
HLT_IsoMu24_eta2p1
HLT_IsoMu24
HLT_IsoMu27
HLT_IsoTkMu18
HLT_IsoTkMu20
HLT_IsoTkMu22_eta2p1
HLT_IsoTkMu22
HLT_IsoTkMu24_eta2p1
HLT_IsoTkMu24
HLT_IsoTkMu27
HLT_L1SingleMu16
HLT_L1SingleMu18
HLT_L2Mu10
HLT_Mu10_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT350_PFMETNoMu60
HLT_Mu15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Mu15_IsoVVVL_PFHT350_PFMET50
HLT_Mu15_IsoVVVL_PFHT350
HLT_Mu15_IsoVVVL_PFHT400_PFMET50
HLT_Mu15_IsoVVVL_PFHT400
HLT_Mu15_IsoVVVL_PFHT600
HLT_Mu16_eta2p1_MET30
HLT_Mu20
HLT_Mu24_eta2p1
HLT_Mu27
HLT_Mu28NoFiltersNoVtx_CentralCaloJet40
HLT_Mu28NoFiltersNoVtx_DisplacedJet40_Loose
HLT_Mu300
HLT_Mu30_eta2p1_PFJet150_PFJet50
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Loose
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Tight
HLT_Mu350
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Loose
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Tight
HLT_Mu38NoFiltersNoVtx_DisplacedJet60_Loose
HLT_Mu40_eta2p1_PFJet200_PFJet50
HLT_Mu45_eta2p1
HLT_Mu50_IsoVVVL_PFHT400
HLT_Mu50
HLT_Mu55
HLT_Mu8_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT300_PFMETNoMu60
HLT_TkMu17
HLT_TkMu20
HLT_TkMu24_eta2p1
HLT_TkMu27
HLT_TkMu50

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one energetic muon, or at least one muon and one or more jets, tau or high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-SingleMuon-UL2016_MiniAODv2
Output dataset: /SingleMuon/Run2016G-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_SingleMuon
Output dataset: /SingleMuon/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleIsoMu17_eta2p1_noDzCut
HLT_DoubleIsoMu17_eta2p1
HLT_IsoMu16_eta2p1_MET30_LooseIsoPFTau50_Trk30_eta2p1
HLT_IsoMu16_eta2p1_MET30
HLT_IsoMu17_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu17_eta2p1_LooseIsoPFTau20
HLT_IsoMu18
HLT_IsoMu19_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu19_eta2p1_LooseIsoPFTau20
HLT_IsoMu19_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu20
HLT_IsoMu21_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu21_eta2p1_LooseIsoPFTau50_Trk30_eta2p1_SingleL1
HLT_IsoMu21_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu22_eta2p1
HLT_IsoMu22
HLT_IsoMu24_eta2p1
HLT_IsoMu24
HLT_IsoMu27
HLT_IsoTkMu18
HLT_IsoTkMu20
HLT_IsoTkMu22_eta2p1
HLT_IsoTkMu22
HLT_IsoTkMu24_eta2p1
HLT_IsoTkMu24
HLT_IsoTkMu27
HLT_L1SingleMu16
HLT_L1SingleMu18
HLT_L2Mu10
HLT_Mu10_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT350_PFMETNoMu60
HLT_Mu15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Mu15_IsoVVVL_PFHT350_PFMET50
HLT_Mu15_IsoVVVL_PFHT350
HLT_Mu15_IsoVVVL_PFHT400_PFMET50
HLT_Mu15_IsoVVVL_PFHT400
HLT_Mu15_IsoVVVL_PFHT600
HLT_Mu16_eta2p1_MET30
HLT_Mu20
HLT_Mu24_eta2p1
HLT_Mu27
HLT_Mu28NoFiltersNoVtx_CentralCaloJet40
HLT_Mu28NoFiltersNoVtx_DisplacedJet40_Loose
HLT_Mu300
HLT_Mu30_eta2p1_PFJet150_PFJet50
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Loose
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Tight
HLT_Mu350
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Loose
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Tight
HLT_Mu38NoFiltersNoVtx_DisplacedJet60_Loose
HLT_Mu40_eta2p1_PFJet200_PFJet50
HLT_Mu45_eta2p1
HLT_Mu50_IsoVVVL_PFHT400
HLT_Mu50
HLT_Mu55
HLT_Mu8_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT300_PFMETNoMu60
HLT_TkMu17
HLT_TkMu20
HLT_TkMu24_eta2p1
HLT_TkMu27
HLT_TkMu50

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -3941,15 +3941,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -4083,7 +4083,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-SinglePhoton-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon120_R9Id90_HE10_IsoM
HLT_Photon120
HLT_Photon135_PFMET100
HLT_Photon165_HE10
HLT_Photon165_R9Id90_HE10_IsoM
HLT_Photon175
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon22_R9Id90_HE10_IsoM
HLT_Photon22
HLT_Photon250_NoHE
HLT_Photon300_NoHE
HLT_Photon30_R9Id90_HE10_IsoM
HLT_Photon30
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon36_R9Id90_HE10_IsoM
HLT_Photon36
HLT_Photon500
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon50_R9Id90_HE10_IsoM
HLT_Photon50
HLT_Photon600
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon75_R9Id90_HE10_IsoM
HLT_Photon75
HLT_Photon90_CaloIdL_PFHT500
HLT_Photon90_CaloIdL_PFHT600
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon90_R9Id90_HE10_IsoM
HLT_Photon90

" + "description": "

Events stored in this primary dataset were selected because of the presence of one energetic photon, or one photon and high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-SinglePhoton-UL2016_MiniAODv2
Output dataset: /SinglePhoton/Run2016G-UL2016_MiniAODv2-v3/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_SinglePhoton
Output dataset: /SinglePhoton/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon120_R9Id90_HE10_IsoM
HLT_Photon120
HLT_Photon135_PFMET100
HLT_Photon165_HE10
HLT_Photon165_R9Id90_HE10_IsoM
HLT_Photon175
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon22_R9Id90_HE10_IsoM
HLT_Photon22
HLT_Photon250_NoHE
HLT_Photon300_NoHE
HLT_Photon30_R9Id90_HE10_IsoM
HLT_Photon30
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon36_R9Id90_HE10_IsoM
HLT_Photon36
HLT_Photon500
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon50_R9Id90_HE10_IsoM
HLT_Photon50
HLT_Photon600
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon75_R9Id90_HE10_IsoM
HLT_Photon75
HLT_Photon90_CaloIdL_PFHT500
HLT_Photon90_CaloIdL_PFHT600
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon90_R9Id90_HE10_IsoM
HLT_Photon90

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -4217,15 +4217,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -4373,7 +4373,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-Tau-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMediumCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1
HLT_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1
HLT_IsoMu19_eta2p1_LooseCombinedIsoPFTau20
HLT_IsoMu19_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu19_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET110
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET120
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET80
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET90
HLT_LooseIsoPFTau50_Trk30_eta2p1
HLT_PFTau120_eta2p1
HLT_PFTau140_eta2p1
HLT_VLooseIsoPFTau120_Trk50_eta2p1
HLT_VLooseIsoPFTau140_Trk50_eta2p1

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one tau, or one tau and muon or high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-Tau-UL2016_MiniAODv2
Output dataset: /Tau/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_Tau
Output dataset: /Tau/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMediumCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1
HLT_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1
HLT_IsoMu19_eta2p1_LooseCombinedIsoPFTau20
HLT_IsoMu19_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu19_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET110
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET120
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET80
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET90
HLT_LooseIsoPFTau50_Trk30_eta2p1
HLT_PFTau120_eta2p1
HLT_PFTau140_eta2p1
HLT_VLooseIsoPFTau120_Trk50_eta2p1
HLT_VLooseIsoPFTau140_Trk50_eta2p1

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -4510,15 +4510,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -4624,7 +4624,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-ZeroBias-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Random

" + "description": "

This primary dataset is an unbiased sample of all collisions.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-ZeroBias-UL2016_MiniAODv2
Output dataset: /ZeroBias/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_ZeroBias
Output dataset: /ZeroBias/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Random

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -4749,15 +4749,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -4797,6 +4797,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30517/BTagCSV_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30517/BTagCSV_doc.html" + }, "date_created": [ "2016" ], @@ -4863,7 +4867,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-BTagCSV-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleJet90_Double30_DoubleBTagCSV_p087
HLT_DoubleJet90_Double30_TripleBTagCSV_p087
HLT_DoubleJetsC100_DoubleBTagCSV_p014_DoublePFJetsC100MaxDeta1p6
HLT_DoubleJetsC100_DoubleBTagCSV_p026_DoublePFJetsC160
HLT_DoubleJetsC100_SingleBTagCSV_p014_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p014
HLT_DoubleJetsC100_SingleBTagCSV_p026_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p026
HLT_DoubleJetsC112_DoubleBTagCSV_p014_DoublePFJetsC112MaxDeta1p6
HLT_DoubleJetsC112_DoubleBTagCSV_p026_DoublePFJetsC172
HLT_QuadJet45_DoubleBTagCSV_p087
HLT_QuadJet45_TripleBTagCSV_p087
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq460
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq500
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq200
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq240
HLT_Rsq0p02_MR300_TriPFJet80_60_40_BTagCSV_p063_p20_Mbb60_200
HLT_Rsq0p02_MR300_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR400_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR450_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR500_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR550_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two jets, tagged as b-quark jets with combined secondary vertex.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-BTagCSV-UL2016_MiniAODv2_NanoAODv9
Output dataset: /BTagCSV/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-BTagCSV-UL2016_MiniAODv2
Output dataset: /BTagCSV/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_BTagCSV
Output dataset: /BTagCSV/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleJet90_Double30_DoubleBTagCSV_p087
HLT_DoubleJet90_Double30_TripleBTagCSV_p087
HLT_DoubleJetsC100_DoubleBTagCSV_p014_DoublePFJetsC100MaxDeta1p6
HLT_DoubleJetsC100_DoubleBTagCSV_p026_DoublePFJetsC160
HLT_DoubleJetsC100_SingleBTagCSV_p014_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p014
HLT_DoubleJetsC100_SingleBTagCSV_p026_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p026
HLT_DoubleJetsC112_DoubleBTagCSV_p014_DoublePFJetsC112MaxDeta1p6
HLT_DoubleJetsC112_DoubleBTagCSV_p026_DoublePFJetsC172
HLT_QuadJet45_DoubleBTagCSV_p087
HLT_QuadJet45_TripleBTagCSV_p087
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq460
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq500
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq200
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq240
HLT_Rsq0p02_MR300_TriPFJet80_60_40_BTagCSV_p063_p20_Mbb60_200
HLT_Rsq0p02_MR300_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR400_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR450_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR500_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR550_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -5043,6 +5047,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30518/BTagMu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30518/BTagMu_doc.html" + }, "date_created": [ "2016" ], @@ -5081,7 +5089,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-BTagMu-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_BTagMu_AK8Jet300_Mu5
HLT_BTagMu_DiJet110_Mu5
HLT_BTagMu_DiJet170_Mu5
HLT_BTagMu_DiJet20_Mu5
HLT_BTagMu_DiJet40_Mu5
HLT_BTagMu_DiJet70_Mu5
HLT_BTagMu_Jet300_Mu5

" + "description": "

Events stored in this primary dataset were selected because of the presence of a muon from the b-quark decay, and one or more jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-BTagMu-UL2016_MiniAODv2_NanoAODv9
Output dataset: /BTagMu/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-BTagMu-UL2016_MiniAODv2
Output dataset: /BTagMu/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_BTagMu
Output dataset: /BTagMu/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_BTagMu_AK8Jet300_Mu5
HLT_BTagMu_DiJet110_Mu5
HLT_BTagMu_DiJet170_Mu5
HLT_BTagMu_DiJet20_Mu5
HLT_BTagMu_DiJet40_Mu5
HLT_BTagMu_DiJet70_Mu5
HLT_BTagMu_Jet300_Mu5

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -5261,6 +5269,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30519/Charmonium_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30519/Charmonium_doc.html" + }, "date_created": [ "2016" ], @@ -5299,7 +5311,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-Charmonium-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Jpsi_Muon
HLT_Dimuon0er16_Jpsi_NoOS_NoVertexing
HLT_Dimuon0er16_Jpsi_NoVertexing
HLT_Dimuon10_Jpsi_Barrel
HLT_Dimuon13_PsiPrime
HLT_Dimuon16_Jpsi
HLT_Dimuon20_Jpsi
HLT_Dimuon6_Jpsi_NoVertexing
HLT_Dimuon8_PsiPrime_Barrel
HLT_DoubleMu4_3_Bs
HLT_DoubleMu4_3_Jpsi_Displaced
HLT_DoubleMu4_JpsiTrk_Displaced
HLT_DoubleMu4_PsiPrimeTrk_Displaced
HLT_Mu7p5_L2Mu2_Jpsi
HLT_Mu7p5_Track2_Jpsi
HLT_Mu7p5_Track3p5_Jpsi
HLT_Mu7p5_Track7_Jpsi
HLT_QuadMuon0_Dimuon0_Jpsi

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons, or a muon and a track with some requirements in the invariant mass for selecting low-mass resonances.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-Charmonium-UL2016_MiniAODv2_NanoAODv9
Output dataset: /Charmonium/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-Charmonium-UL2016_MiniAODv2
Output dataset: /Charmonium/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_Charmonium
Output dataset: /Charmonium/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Jpsi_Muon
HLT_Dimuon0er16_Jpsi_NoOS_NoVertexing
HLT_Dimuon0er16_Jpsi_NoVertexing
HLT_Dimuon10_Jpsi_Barrel
HLT_Dimuon13_PsiPrime
HLT_Dimuon16_Jpsi
HLT_Dimuon20_Jpsi
HLT_Dimuon6_Jpsi_NoVertexing
HLT_Dimuon8_PsiPrime_Barrel
HLT_DoubleMu4_3_Bs
HLT_DoubleMu4_3_Jpsi_Displaced
HLT_DoubleMu4_JpsiTrk_Displaced
HLT_DoubleMu4_PsiPrimeTrk_Displaced
HLT_Mu7p5_L2Mu2_Jpsi
HLT_Mu7p5_Track2_Jpsi
HLT_Mu7p5_Track3p5_Jpsi
HLT_Mu7p5_Track7_Jpsi
HLT_QuadMuon0_Dimuon0_Jpsi

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -5478,6 +5490,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30520/DisplacedJet_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30520/DisplacedJet_doc.html" + }, "date_created": [ "2016" ], @@ -5516,7 +5532,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-DisplacedJet-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_HT200_DisplacedDijet40_DisplacedTrack
HLT_HT200
HLT_HT250_DisplacedDijet40_DisplacedTrack
HLT_HT275
HLT_HT325
HLT_HT350_DisplacedDijet40_DisplacedTrack
HLT_HT350_DisplacedDijet40_Inclusive
HLT_HT350_DisplacedDijet80_DisplacedTrack
HLT_HT350_DisplacedDijet80_Tight_DisplacedTrack
HLT_HT400_DisplacedDijet40_Inclusive
HLT_HT425
HLT_HT500_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet80_Inclusive
HLT_HT575
HLT_HT650_DisplacedDijet80_Inclusive
HLT_HT750_DisplacedDijet80_Inclusive
HLT_VBF_DisplacedJet40_DisplacedTrack_2TrackIP2DSig5
HLT_VBF_DisplacedJet40_DisplacedTrack
HLT_VBF_DisplacedJet40_Hadronic_2PromptTrack
HLT_VBF_DisplacedJet40_Hadronic
HLT_VBF_DisplacedJet40_TightID_DisplacedTrack
HLT_VBF_DisplacedJet40_TightID_Hadronic
HLT_VBF_DisplacedJet40_VTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VTightID_Hadronic
HLT_VBF_DisplacedJet40_VVTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VVTightID_Hadronic

" + "description": "

Events stored in this primary dataset were selected because of the presence of one or more displaced jets, or a displaced jet and/or high scalar sum of the jet transverse momenta (HT).

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-DisplacedJet-UL2016_MiniAODv2_NanoAODv9
Output dataset: /DisplacedJet/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DisplacedJet-UL2016_MiniAODv2
Output dataset: /DisplacedJet/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_DisplacedJet
Output dataset: /DisplacedJet/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_HT200_DisplacedDijet40_DisplacedTrack
HLT_HT200
HLT_HT250_DisplacedDijet40_DisplacedTrack
HLT_HT275
HLT_HT325
HLT_HT350_DisplacedDijet40_DisplacedTrack
HLT_HT350_DisplacedDijet40_Inclusive
HLT_HT350_DisplacedDijet80_DisplacedTrack
HLT_HT350_DisplacedDijet80_Tight_DisplacedTrack
HLT_HT400_DisplacedDijet40_Inclusive
HLT_HT425
HLT_HT500_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet80_Inclusive
HLT_HT575
HLT_HT650_DisplacedDijet80_Inclusive
HLT_HT750_DisplacedDijet80_Inclusive
HLT_VBF_DisplacedJet40_DisplacedTrack_2TrackIP2DSig5
HLT_VBF_DisplacedJet40_DisplacedTrack
HLT_VBF_DisplacedJet40_Hadronic_2PromptTrack
HLT_VBF_DisplacedJet40_Hadronic
HLT_VBF_DisplacedJet40_TightID_DisplacedTrack
HLT_VBF_DisplacedJet40_TightID_Hadronic
HLT_VBF_DisplacedJet40_VTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VTightID_Hadronic
HLT_VBF_DisplacedJet40_VVTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VVTightID_Hadronic

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -5696,6 +5712,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30521/DoubleEG_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30521/DoubleEG_doc.html" + }, "date_created": [ "2016" ], @@ -5762,7 +5782,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-DoubleEG-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Diphoton30EB_18EB_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30PV_18PV_R9Id_AND_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelSeedMatch_Mass70
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_Mass90
HLT_Diphoton30_18_Solid_R9Id_AND_IsoCaloId_AND_HE_R9Id_Mass55
HLT_DoubleEle24_22_eta2p1_WPLoose_Gsf
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL_MW
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL
HLT_DoubleEle33_CaloIdL_MW
HLT_DoubleEle33_CaloIdL
HLT_DoubleEle37_Ele27_CaloIdL_GsfTrkIdVL
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_DoublePhoton60
HLT_DoublePhoton85
HLT_ECALHT800
HLT_Ele10_CaloIdM_TrackIdM_CentralPFJet30_BTagCSV_p13
HLT_Ele12_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele12_CaloIdM_TrackIdM_PFJet30
HLT_Ele16_Ele12_Ele8_CaloIdL_TrackIdL
HLT_Ele17_CaloIdL_GsfTrkIdVL
HLT_Ele17_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Ele17_CaloIdM_TrackIdM_PFJet30
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdM_TrackIdM_PFJet30
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ_L1JetTauSeeded
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele27_HighEta_Ele20_Mass55
HLT_Ele30WP60_Ele8_Mass55
HLT_Ele30WP60_SC4_Mass55
HLT_Ele8_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele8_CaloIdM_TrackIdM_PFJet30
HLT_Photon26_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon16_AND_HE10_R9Id65_Eta2_Mass60
HLT_Photon36_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon22_AND_HE10_R9Id65_Eta2_Mass15
HLT_Photon42_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon25_AND_HE10_R9Id65_Eta2_Mass15

" + "description": "

Events stored in this primary dataset were selected because of the presence of different combinations of energetic photons, electrons and/or jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-DoubleEG-UL2016_MiniAODv2_NanoAODv9
Output dataset: /DoubleEG/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DoubleEG-UL2016_MiniAODv2
Output dataset: /DoubleEG/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_DoubleEG
Output dataset: /DoubleEG/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Diphoton30EB_18EB_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30PV_18PV_R9Id_AND_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelSeedMatch_Mass70
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_Mass90
HLT_Diphoton30_18_Solid_R9Id_AND_IsoCaloId_AND_HE_R9Id_Mass55
HLT_DoubleEle24_22_eta2p1_WPLoose_Gsf
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL_MW
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL
HLT_DoubleEle33_CaloIdL_MW
HLT_DoubleEle33_CaloIdL
HLT_DoubleEle37_Ele27_CaloIdL_GsfTrkIdVL
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_DoublePhoton60
HLT_DoublePhoton85
HLT_ECALHT800
HLT_Ele10_CaloIdM_TrackIdM_CentralPFJet30_BTagCSV_p13
HLT_Ele12_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele12_CaloIdM_TrackIdM_PFJet30
HLT_Ele16_Ele12_Ele8_CaloIdL_TrackIdL
HLT_Ele17_CaloIdL_GsfTrkIdVL
HLT_Ele17_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Ele17_CaloIdM_TrackIdM_PFJet30
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdM_TrackIdM_PFJet30
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ_L1JetTauSeeded
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele27_HighEta_Ele20_Mass55
HLT_Ele30WP60_Ele8_Mass55
HLT_Ele30WP60_SC4_Mass55
HLT_Ele8_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele8_CaloIdM_TrackIdM_PFJet30
HLT_Photon26_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon16_AND_HE10_R9Id65_Eta2_Mass60
HLT_Photon36_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon22_AND_HE10_R9Id65_Eta2_Mass15
HLT_Photon42_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon25_AND_HE10_R9Id65_Eta2_Mass15

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -5939,6 +5959,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30522/DoubleMuon_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30522/DoubleMuon_doc.html" + }, "date_created": [ "2016" ], @@ -5977,7 +6001,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-DoubleMuon-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu0
HLT_DoubleMu18NoFiltersNoVtx
HLT_DoubleMu23NoFiltersNoVtxDisplaced
HLT_DoubleMu28NoFiltersNoVtxDisplaced
HLT_DoubleMu33NoFiltersNoVtx
HLT_DoubleMu38NoFiltersNoVtx
HLT_DoubleMu8_Mass8_PFHT250
HLT_DoubleMu8_Mass8_PFHT300
HLT_L2DoubleMu23_NoVertex
HLT_L2DoubleMu28_NoVertex_2Cha_Angle2p5_Mass10
HLT_L2DoubleMu38_NoVertex_2Cha_Angle2p5_Mass10
HLT_Mu10_CentralPFJet30_BTagCSV_p13
HLT_Mu17_Mu8_DZ
HLT_Mu17_Mu8_SameSign_DZ
HLT_Mu17_Mu8_SameSign
HLT_Mu17_Mu8
HLT_Mu17_TkMu8_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL
HLT_Mu17
HLT_Mu20_Mu10_DZ
HLT_Mu20_Mu10_SameSign_DZ
HLT_Mu20_Mu10_SameSign
HLT_Mu20_Mu10
HLT_Mu27_TkMu8
HLT_Mu30_TkMu11
HLT_Mu3_PFJet40
HLT_Mu40_TkMu11
HLT_Mu8_TrkIsoVVL
HLT_Mu8
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_TripleMu_12_10_5
HLT_TripleMu_5_3_3_DZ_Mass3p8
HLT_TripleMu_5_3_3
HLT_TrkMu15_DoubleTrkMu5NoFiltersNoVtx
HLT_TrkMu17_DoubleTrkMu8NoFiltersNoVtx

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two energetic muons in the event.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-DoubleMuon-UL2016_MiniAODv2_NanoAODv9
Output dataset: /DoubleMuon/Run2016G-UL2016_MiniAODv2_NanoAODv9-v2/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DoubleMuon-UL2016_MiniAODv2
Output dataset: /DoubleMuon/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_DoubleMuon
Output dataset: /DoubleMuon/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu0
HLT_DoubleMu18NoFiltersNoVtx
HLT_DoubleMu23NoFiltersNoVtxDisplaced
HLT_DoubleMu28NoFiltersNoVtxDisplaced
HLT_DoubleMu33NoFiltersNoVtx
HLT_DoubleMu38NoFiltersNoVtx
HLT_DoubleMu8_Mass8_PFHT250
HLT_DoubleMu8_Mass8_PFHT300
HLT_L2DoubleMu23_NoVertex
HLT_L2DoubleMu28_NoVertex_2Cha_Angle2p5_Mass10
HLT_L2DoubleMu38_NoVertex_2Cha_Angle2p5_Mass10
HLT_Mu10_CentralPFJet30_BTagCSV_p13
HLT_Mu17_Mu8_DZ
HLT_Mu17_Mu8_SameSign_DZ
HLT_Mu17_Mu8_SameSign
HLT_Mu17_Mu8
HLT_Mu17_TkMu8_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL
HLT_Mu17
HLT_Mu20_Mu10_DZ
HLT_Mu20_Mu10_SameSign_DZ
HLT_Mu20_Mu10_SameSign
HLT_Mu20_Mu10
HLT_Mu27_TkMu8
HLT_Mu30_TkMu11
HLT_Mu3_PFJet40
HLT_Mu40_TkMu11
HLT_Mu8_TrkIsoVVL
HLT_Mu8
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_TripleMu_12_10_5
HLT_TripleMu_5_3_3_DZ_Mass3p8
HLT_TripleMu_5_3_3
HLT_TrkMu15_DoubleTrkMu5NoFiltersNoVtx
HLT_TrkMu17_DoubleTrkMu8NoFiltersNoVtx

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -6156,6 +6180,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30523/DoubleMuonLowMass_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30523/DoubleMuonLowMass_doc.html" + }, "date_created": [ "2016" ], @@ -6194,7 +6222,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-DoubleMuonLowMass-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu3_Trk_Tau3mu
HLT_DoubleMu4_LowMassNonResonantTrk_Displaced

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons with low invariant mass.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-DoubleMuonLowMass-UL2016_MiniAODv2_NanoAODv9
Output dataset: /DoubleMuonLowMass/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-DoubleMuonLowMass-UL2016_MiniAODv2
Output dataset: /DoubleMuonLowMass/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step ReReco-Run2016G-DoubleMuonLowMass-21Feb2020_UL2016
Output dataset: /DoubleMuonLowMass/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu3_Trk_Tau3mu
HLT_DoubleMu4_LowMassNonResonantTrk_Displaced

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -6373,6 +6401,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30524/HTMHT_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30524/HTMHT_doc.html" + }, "date_created": [ "2016" ], @@ -6411,7 +6443,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-HTMHT-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu140
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu80
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p57
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p63
HLT_PFHT200_PFAlphaT0p51
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p55
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p58
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p54
HLT_PFHT300_PFMET100
HLT_PFHT300_PFMET110
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p52
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p51
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p52
HLT_Rsq0p25
HLT_Rsq0p30
HLT_RsqMR240_Rsq0p09_MR200_4jet
HLT_RsqMR240_Rsq0p09_MR200
HLT_RsqMR270_Rsq0p09_MR200_4jet
HLT_RsqMR270_Rsq0p09_MR200

" + "description": "

Events stored in this primary dataset were selected because of the presence of a combination of a high scalar sum of the jet transverse momenta (HT), one or more energetic jets, or high missing transverse energy.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-HTMHT-UL2016_MiniAODv2_NanoAODv9
Output dataset: /HTMHT/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-HTMHT-UL2016_MiniAODv2
Output dataset: /HTMHT/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_HTMHT
Output dataset: /HTMHT/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu140
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu80
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p57
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p63
HLT_PFHT200_PFAlphaT0p51
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p55
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p58
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p54
HLT_PFHT300_PFMET100
HLT_PFHT300_PFMET110
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p52
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p51
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p52
HLT_Rsq0p25
HLT_Rsq0p30
HLT_RsqMR240_Rsq0p09_MR200_4jet
HLT_RsqMR240_Rsq0p09_MR200
HLT_RsqMR270_Rsq0p09_MR200_4jet
HLT_RsqMR270_Rsq0p09_MR200

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -6590,6 +6622,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30525/JetHT_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30525/JetHT_doc.html" + }, "date_created": [ "2016" ], @@ -6642,7 +6678,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-JetHT-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_AK8DiPFJet250_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet250_200_TrimMass30
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet280_200_TrimMass30
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet300_200_TrimMass30
HLT_AK8PFHT600_TrimR0p1PT0p03Mass50_BTagCSV_p20
HLT_AK8PFHT650_TrimR0p1PT0p03Mass50
HLT_AK8PFHT700_TrimR0p1PT0p03Mass50
HLT_AK8PFHT750_TrimMass50
HLT_AK8PFHT800_TrimMass50
HLT_AK8PFJet140
HLT_AK8PFJet200
HLT_AK8PFJet260
HLT_AK8PFJet320
HLT_AK8PFJet360_TrimMass30
HLT_AK8PFJet400_TrimMass30
HLT_AK8PFJet400
HLT_AK8PFJet40
HLT_AK8PFJet450
HLT_AK8PFJet500
HLT_AK8PFJet60
HLT_AK8PFJet80
HLT_CaloJet500_NoJetID
HLT_DiCentralPFJet170_CFMax0p1
HLT_DiCentralPFJet170
HLT_DiCentralPFJet220_CFMax0p3
HLT_DiCentralPFJet330_CFMax0p5
HLT_DiCentralPFJet430
HLT_DiJetVBFMu_PassThrough
HLT_DiJetVBF_PassThrough
HLT_DiPFJetAve100_HFJEC
HLT_DiPFJetAve140
HLT_DiPFJetAve160_HFJEC
HLT_DiPFJetAve200
HLT_DiPFJetAve220_HFJEC
HLT_DiPFJetAve260
HLT_DiPFJetAve300_HFJEC
HLT_DiPFJetAve320
HLT_DiPFJetAve400
HLT_DiPFJetAve40
HLT_DiPFJetAve500
HLT_DiPFJetAve60_HFJEC
HLT_DiPFJetAve60
HLT_DiPFJetAve80_HFJEC
HLT_DiPFJetAve80
HLT_HT2000
HLT_HT2500
HLT_L1_TripleJet_VBF
HLT_PFHT125
HLT_PFHT200
HLT_PFHT250
HLT_PFHT300
HLT_PFHT350
HLT_PFHT400_SixJet30_DoubleBTagCSV_p056
HLT_PFHT400_SixJet30
HLT_PFHT400
HLT_PFHT450_SixJet40_BTagCSV_p056
HLT_PFHT450_SixJet40
HLT_PFHT475
HLT_PFHT550_4JetPt50
HLT_PFHT600
HLT_PFHT650_4JetPt50
HLT_PFHT650_WideJetMJJ900DEtaJJ1p5
HLT_PFHT650_WideJetMJJ950DEtaJJ1p5
HLT_PFHT650
HLT_PFHT750_4JetPt50
HLT_PFHT750_4JetPt70
HLT_PFHT750_4JetPt80
HLT_PFHT800_4JetPt50
HLT_PFHT800
HLT_PFHT850_4JetPt50
HLT_PFHT900
HLT_PFJet140
HLT_PFJet200
HLT_PFJet260
HLT_PFJet320
HLT_PFJet400
HLT_PFJet40
HLT_PFJet450
HLT_PFJet500
HLT_PFJet60
HLT_PFJet80
HLT_QuadPFJet_VBF
HLT_SingleCentralPFJet170_CFMax0p1

" + "description": "

Events stored in this primary dataset were selected because of the presence of a high scalar sum of the jet transverse momenta (HT), or at least one or two energetic jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-JetHT-UL2016_MiniAODv2_NanoAODv9
Output dataset: /JetHT/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-JetHT-UL2016_MiniAODv2
Output dataset: /JetHT/Run2016G-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_JetHT
Output dataset: /JetHT/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_AK8DiPFJet250_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet250_200_TrimMass30
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet280_200_TrimMass30
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet300_200_TrimMass30
HLT_AK8PFHT600_TrimR0p1PT0p03Mass50_BTagCSV_p20
HLT_AK8PFHT650_TrimR0p1PT0p03Mass50
HLT_AK8PFHT700_TrimR0p1PT0p03Mass50
HLT_AK8PFHT750_TrimMass50
HLT_AK8PFHT800_TrimMass50
HLT_AK8PFJet140
HLT_AK8PFJet200
HLT_AK8PFJet260
HLT_AK8PFJet320
HLT_AK8PFJet360_TrimMass30
HLT_AK8PFJet400_TrimMass30
HLT_AK8PFJet400
HLT_AK8PFJet40
HLT_AK8PFJet450
HLT_AK8PFJet500
HLT_AK8PFJet60
HLT_AK8PFJet80
HLT_CaloJet500_NoJetID
HLT_DiCentralPFJet170_CFMax0p1
HLT_DiCentralPFJet170
HLT_DiCentralPFJet220_CFMax0p3
HLT_DiCentralPFJet330_CFMax0p5
HLT_DiCentralPFJet430
HLT_DiJetVBFMu_PassThrough
HLT_DiJetVBF_PassThrough
HLT_DiPFJetAve100_HFJEC
HLT_DiPFJetAve140
HLT_DiPFJetAve160_HFJEC
HLT_DiPFJetAve200
HLT_DiPFJetAve220_HFJEC
HLT_DiPFJetAve260
HLT_DiPFJetAve300_HFJEC
HLT_DiPFJetAve320
HLT_DiPFJetAve400
HLT_DiPFJetAve40
HLT_DiPFJetAve500
HLT_DiPFJetAve60_HFJEC
HLT_DiPFJetAve60
HLT_DiPFJetAve80_HFJEC
HLT_DiPFJetAve80
HLT_HT2000
HLT_HT2500
HLT_L1_TripleJet_VBF
HLT_PFHT125
HLT_PFHT200
HLT_PFHT250
HLT_PFHT300
HLT_PFHT350
HLT_PFHT400_SixJet30_DoubleBTagCSV_p056
HLT_PFHT400_SixJet30
HLT_PFHT400
HLT_PFHT450_SixJet40_BTagCSV_p056
HLT_PFHT450_SixJet40
HLT_PFHT475
HLT_PFHT550_4JetPt50
HLT_PFHT600
HLT_PFHT650_4JetPt50
HLT_PFHT650_WideJetMJJ900DEtaJJ1p5
HLT_PFHT650_WideJetMJJ950DEtaJJ1p5
HLT_PFHT650
HLT_PFHT750_4JetPt50
HLT_PFHT750_4JetPt70
HLT_PFHT750_4JetPt80
HLT_PFHT800_4JetPt50
HLT_PFHT800
HLT_PFHT850_4JetPt50
HLT_PFHT900
HLT_PFJet140
HLT_PFJet200
HLT_PFJet260
HLT_PFJet320
HLT_PFJet400
HLT_PFJet40
HLT_PFJet450
HLT_PFJet500
HLT_PFJet60
HLT_PFJet80
HLT_QuadPFJet_VBF
HLT_SingleCentralPFJet170_CFMax0p1

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -6821,6 +6857,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30526/MET_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30526/MET_doc.html" + }, "date_created": [ "2016" ], @@ -6873,7 +6913,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-MET-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight_BTagCSV_p067
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight
HLT_DiCentralPFJet55_PFMET110
HLT_DoubleMu3_PFMET50
HLT_MET200
HLT_MET250
HLT_MET300
HLT_MET600
HLT_MET60_IsoTrk35_Loose
HLT_MET700
HLT_MET75_IsoTrk50
HLT_MET90_IsoTrk50
HLT_MonoCentralPFJet80_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_Mu14er_PFMET100
HLT_Mu3er_PFHT140_PFMET125
HLT_Mu6_PFHT200_PFMET100
HLT_Mu6_PFHT200_PFMET80_BTagCSV_p067
HLT_PFMET100_PFMHT100_IDTight_BeamHaloCleaned
HLT_PFMET100_PFMHT100_IDTight
HLT_PFMET110_PFMHT110_IDTight
HLT_PFMET120_BTagCSV_p067
HLT_PFMET120_Mu5
HLT_PFMET120_PFMHT120_IDTight
HLT_PFMET170_BeamHaloCleaned
HLT_PFMET170_HBHECleaned
HLT_PFMET170_HBHE_BeamHaloCleaned
HLT_PFMET170_JetIdCleaned
HLT_PFMET170_NoiseCleaned
HLT_PFMET170_NotCleaned
HLT_PFMET300
HLT_PFMET400
HLT_PFMET500
HLT_PFMET600
HLT_PFMET90_PFMHT90_IDTight
HLT_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_PFMETTypeOne190_HBHE_BeamHaloCleaned

" + "description": "

Events stored in this primary dataset were selected because of the presence of high missing transverse energy.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-MET-UL2016_MiniAODv2_NanoAODv9
Output dataset: /MET/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-MET-UL2016_MiniAODv2
Output dataset: /MET/Run2016G-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_MET
Output dataset: /MET/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight_BTagCSV_p067
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight
HLT_DiCentralPFJet55_PFMET110
HLT_DoubleMu3_PFMET50
HLT_MET200
HLT_MET250
HLT_MET300
HLT_MET600
HLT_MET60_IsoTrk35_Loose
HLT_MET700
HLT_MET75_IsoTrk50
HLT_MET90_IsoTrk50
HLT_MonoCentralPFJet80_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_Mu14er_PFMET100
HLT_Mu3er_PFHT140_PFMET125
HLT_Mu6_PFHT200_PFMET100
HLT_Mu6_PFHT200_PFMET80_BTagCSV_p067
HLT_PFMET100_PFMHT100_IDTight_BeamHaloCleaned
HLT_PFMET100_PFMHT100_IDTight
HLT_PFMET110_PFMHT110_IDTight
HLT_PFMET120_BTagCSV_p067
HLT_PFMET120_Mu5
HLT_PFMET120_PFMHT120_IDTight
HLT_PFMET170_BeamHaloCleaned
HLT_PFMET170_HBHECleaned
HLT_PFMET170_HBHE_BeamHaloCleaned
HLT_PFMET170_JetIdCleaned
HLT_PFMET170_NoiseCleaned
HLT_PFMET170_NotCleaned
HLT_PFMET300
HLT_PFMET400
HLT_PFMET500
HLT_PFMET600
HLT_PFMET90_PFMHT90_IDTight
HLT_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_PFMETTypeOne190_HBHE_BeamHaloCleaned

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -7053,6 +7093,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30527/MuOnia_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30527/MuOnia_doc.html" + }, "date_created": [ "2016" ], @@ -7105,7 +7149,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-MuOnia-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Phi_Barrel
HLT_Dimuon0_Upsilon_Muon
HLT_Dimuon13_Upsilon
HLT_Dimuon8_Upsilon_Barrel
HLT_Mu16_TkMu0_dEta18_Onia
HLT_Mu16_TkMu0_dEta18_Phi
HLT_Mu25_TkMu0_dEta18_Onia
HLT_Mu7p5_L2Mu2_Upsilon
HLT_Mu7p5_Track2_Upsilon
HLT_Mu7p5_Track3p5_Upsilon
HLT_Mu7p5_Track7_Upsilon
HLT_QuadMuon0_Dimuon0_Upsilon

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons in the event requiring only very low energy and some requirements in the invariant mass for selecting low-mass resonances.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-MuOnia-UL2016_MiniAODv2_NanoAODv9
Output dataset: /MuOnia/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-MuOnia-UL2016_MiniAODv2
Output dataset: /MuOnia/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_MuOnia
Output dataset: /MuOnia/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Phi_Barrel
HLT_Dimuon0_Upsilon_Muon
HLT_Dimuon13_Upsilon
HLT_Dimuon8_Upsilon_Barrel
HLT_Mu16_TkMu0_dEta18_Onia
HLT_Mu16_TkMu0_dEta18_Phi
HLT_Mu25_TkMu0_dEta18_Onia
HLT_Mu7p5_L2Mu2_Upsilon
HLT_Mu7p5_Track2_Upsilon
HLT_Mu7p5_Track3p5_Upsilon
HLT_Mu7p5_Track7_Upsilon
HLT_QuadMuon0_Dimuon0_Upsilon

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -7284,6 +7328,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30528/MuonEG_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30528/MuonEG_doc.html" + }, "date_created": [ "2016" ], @@ -7350,7 +7398,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-MuonEG-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiMu9_Ele9_CaloIdL_TrackIdL
HLT_Mu12_Photon25_CaloIdL_L1ISO
HLT_Mu12_Photon25_CaloIdL_L1OR
HLT_Mu12_Photon25_CaloIdL
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Mu17_Photon22_CaloIdL_L1ISO
HLT_Mu17_Photon30_CaloIdL_L1ISO
HLT_Mu17_Photon35_CaloIdL_L1ISO
HLT_Mu17_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23NoFiltersNoVtx_Photon23_CaloIdL
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL
HLT_Mu27_Ele37_CaloIdL_GsfTrkIdVL
HLT_Mu28NoFiltersNoVtxDisplaced_Photon28_CaloIdL
HLT_Mu30_Ele30_CaloIdL_GsfTrkIdVL
HLT_Mu33NoFiltersNoVtxDisplaced_Photon33_CaloIdL
HLT_Mu33_Ele33_CaloIdL_GsfTrkIdVL
HLT_Mu37_Ele27_CaloIdL_GsfTrkIdVL
HLT_Mu38NoFiltersNoVtx_Photon38_CaloIdL
HLT_Mu42NoFiltersNoVtx_Photon42_CaloIdL
HLT_Mu8_DiEle12_CaloIdL_TrackIdL
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_Mu8_TrkIsoVVL_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL

" + "description": "

Events stored in this primary dataset were selected because of the presence of one energetic muon and electron or photon.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-MuonEG-UL2016_MiniAODv2_NanoAODv9
Output dataset: /MuonEG/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-MuonEG-UL2016_MiniAODv2
Output dataset: /MuonEG/Run2016G-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_MuonEG
Output dataset: /MuonEG/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiMu9_Ele9_CaloIdL_TrackIdL
HLT_Mu12_Photon25_CaloIdL_L1ISO
HLT_Mu12_Photon25_CaloIdL_L1OR
HLT_Mu12_Photon25_CaloIdL
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Mu17_Photon22_CaloIdL_L1ISO
HLT_Mu17_Photon30_CaloIdL_L1ISO
HLT_Mu17_Photon35_CaloIdL_L1ISO
HLT_Mu17_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23NoFiltersNoVtx_Photon23_CaloIdL
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL
HLT_Mu27_Ele37_CaloIdL_GsfTrkIdVL
HLT_Mu28NoFiltersNoVtxDisplaced_Photon28_CaloIdL
HLT_Mu30_Ele30_CaloIdL_GsfTrkIdVL
HLT_Mu33NoFiltersNoVtxDisplaced_Photon33_CaloIdL
HLT_Mu33_Ele33_CaloIdL_GsfTrkIdVL
HLT_Mu37_Ele27_CaloIdL_GsfTrkIdVL
HLT_Mu38NoFiltersNoVtx_Photon38_CaloIdL
HLT_Mu42NoFiltersNoVtx_Photon42_CaloIdL
HLT_Mu8_DiEle12_CaloIdL_TrackIdL
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_Mu8_TrkIsoVVL_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -7529,6 +7577,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30529/SingleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30529/SingleElectron_doc.html" + }, "date_created": [ "2016" ], @@ -7595,7 +7647,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-SingleElectron-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Ele105_CaloIdVT_GsfTrkIdT
HLT_Ele115_CaloIdVT_GsfTrkIdT
HLT_Ele145_CaloIdVT_GsfTrkIdT
HLT_Ele15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Ele15_IsoVVVL_PFHT350_PFMET50
HLT_Ele15_IsoVVVL_PFHT350
HLT_Ele15_IsoVVVL_PFHT400_PFMET50
HLT_Ele15_IsoVVVL_PFHT400
HLT_Ele15_IsoVVVL_PFHT600
HLT_Ele200_CaloIdVT_GsfTrkIdT
HLT_Ele20_eta2p1_WPLoose_Gsf_LooseIsoPFTau28
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau29
HLT_Ele22_eta2p1_WPLoose_Gsf
HLT_Ele23_WPLoose_Gsf_WHbbBoost
HLT_Ele23_WPLoose_Gsf
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau30
HLT_Ele24_eta2p1_WPLoose_Gsf
HLT_Ele250_CaloIdVT_GsfTrkIdT
HLT_Ele25_WPTight_Gsf
HLT_Ele25_eta2p1_WPLoose_Gsf
HLT_Ele25_eta2p1_WPTight_Gsf
HLT_Ele27_WPLoose_Gsf_WHbbBoost
HLT_Ele27_WPLoose_Gsf
HLT_Ele27_WPTight_Gsf_L1JetTauSeeded
HLT_Ele27_WPTight_Gsf
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_HT200
HLT_Ele27_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele27_eta2p1_WPLoose_Gsf
HLT_Ele27_eta2p1_WPTight_Gsf
HLT_Ele300_CaloIdVT_GsfTrkIdT
HLT_Ele30_WPTight_Gsf
HLT_Ele30_eta2p1_WPTight_Gsf
HLT_Ele32_WPTight_Gsf
HLT_Ele32_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele32_eta2p1_WPTight_Gsf
HLT_Ele35_CaloIdVT_GsfTrkIdT_PFJet150_PFJet50
HLT_Ele35_WPLoose_Gsf
HLT_Ele36_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele45_CaloIdVT_GsfTrkIdT_PFJet200_PFJet50
HLT_Ele45_WPLoose_Gsf_L1JetTauSeeded
HLT_Ele45_WPLoose_Gsf
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet140
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet165
HLT_Ele50_IsoVVVL_PFHT400

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one high-energy electron, or at least one high-energy electron and one or more jets or tau.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-SingleElectron-UL2016_MiniAODv2_NanoAODv9
Output dataset: /SingleElectron/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-SingleElectron-UL2016_MiniAODv2
Output dataset: /SingleElectron/Run2016G-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_SingleElectron
Output dataset: /SingleElectron/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Ele105_CaloIdVT_GsfTrkIdT
HLT_Ele115_CaloIdVT_GsfTrkIdT
HLT_Ele145_CaloIdVT_GsfTrkIdT
HLT_Ele15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Ele15_IsoVVVL_PFHT350_PFMET50
HLT_Ele15_IsoVVVL_PFHT350
HLT_Ele15_IsoVVVL_PFHT400_PFMET50
HLT_Ele15_IsoVVVL_PFHT400
HLT_Ele15_IsoVVVL_PFHT600
HLT_Ele200_CaloIdVT_GsfTrkIdT
HLT_Ele20_eta2p1_WPLoose_Gsf_LooseIsoPFTau28
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau29
HLT_Ele22_eta2p1_WPLoose_Gsf
HLT_Ele23_WPLoose_Gsf_WHbbBoost
HLT_Ele23_WPLoose_Gsf
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau30
HLT_Ele24_eta2p1_WPLoose_Gsf
HLT_Ele250_CaloIdVT_GsfTrkIdT
HLT_Ele25_WPTight_Gsf
HLT_Ele25_eta2p1_WPLoose_Gsf
HLT_Ele25_eta2p1_WPTight_Gsf
HLT_Ele27_WPLoose_Gsf_WHbbBoost
HLT_Ele27_WPLoose_Gsf
HLT_Ele27_WPTight_Gsf_L1JetTauSeeded
HLT_Ele27_WPTight_Gsf
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_HT200
HLT_Ele27_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele27_eta2p1_WPLoose_Gsf
HLT_Ele27_eta2p1_WPTight_Gsf
HLT_Ele300_CaloIdVT_GsfTrkIdT
HLT_Ele30_WPTight_Gsf
HLT_Ele30_eta2p1_WPTight_Gsf
HLT_Ele32_WPTight_Gsf
HLT_Ele32_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele32_eta2p1_WPTight_Gsf
HLT_Ele35_CaloIdVT_GsfTrkIdT_PFJet150_PFJet50
HLT_Ele35_WPLoose_Gsf
HLT_Ele36_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele45_CaloIdVT_GsfTrkIdT_PFJet200_PFJet50
HLT_Ele45_WPLoose_Gsf_L1JetTauSeeded
HLT_Ele45_WPLoose_Gsf
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet140
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet165
HLT_Ele50_IsoVVVL_PFHT400

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -7772,6 +7824,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30530/SingleMuon_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30530/SingleMuon_doc.html" + }, "date_created": [ "2016" ], @@ -7824,7 +7880,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-SingleMuon-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleIsoMu17_eta2p1_noDzCut
HLT_DoubleIsoMu17_eta2p1
HLT_IsoMu16_eta2p1_MET30_LooseIsoPFTau50_Trk30_eta2p1
HLT_IsoMu16_eta2p1_MET30
HLT_IsoMu17_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu17_eta2p1_LooseIsoPFTau20
HLT_IsoMu18
HLT_IsoMu19_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu19_eta2p1_LooseIsoPFTau20
HLT_IsoMu19_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu20
HLT_IsoMu21_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu21_eta2p1_LooseIsoPFTau50_Trk30_eta2p1_SingleL1
HLT_IsoMu21_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu22_eta2p1
HLT_IsoMu22
HLT_IsoMu24_eta2p1
HLT_IsoMu24
HLT_IsoMu27
HLT_IsoTkMu18
HLT_IsoTkMu20
HLT_IsoTkMu22_eta2p1
HLT_IsoTkMu22
HLT_IsoTkMu24_eta2p1
HLT_IsoTkMu24
HLT_IsoTkMu27
HLT_L1SingleMu16
HLT_L1SingleMu18
HLT_L2Mu10
HLT_Mu10_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT350_PFMETNoMu60
HLT_Mu15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Mu15_IsoVVVL_PFHT350_PFMET50
HLT_Mu15_IsoVVVL_PFHT350
HLT_Mu15_IsoVVVL_PFHT400_PFMET50
HLT_Mu15_IsoVVVL_PFHT400
HLT_Mu15_IsoVVVL_PFHT600
HLT_Mu16_eta2p1_MET30
HLT_Mu20
HLT_Mu24_eta2p1
HLT_Mu27
HLT_Mu28NoFiltersNoVtx_CentralCaloJet40
HLT_Mu28NoFiltersNoVtx_DisplacedJet40_Loose
HLT_Mu300
HLT_Mu30_eta2p1_PFJet150_PFJet50
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Loose
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Tight
HLT_Mu350
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Loose
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Tight
HLT_Mu38NoFiltersNoVtx_DisplacedJet60_Loose
HLT_Mu40_eta2p1_PFJet200_PFJet50
HLT_Mu45_eta2p1
HLT_Mu50_IsoVVVL_PFHT400
HLT_Mu50
HLT_Mu55
HLT_Mu8_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT300_PFMETNoMu60
HLT_TkMu17
HLT_TkMu20
HLT_TkMu24_eta2p1
HLT_TkMu27
HLT_TkMu50

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one energetic muon, or at least one muon and one or more jets, tau or high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-SingleMuon-UL2016_MiniAODv2_NanoAODv9
Output dataset: /SingleMuon/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-SingleMuon-UL2016_MiniAODv2
Output dataset: /SingleMuon/Run2016G-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_SingleMuon
Output dataset: /SingleMuon/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleIsoMu17_eta2p1_noDzCut
HLT_DoubleIsoMu17_eta2p1
HLT_IsoMu16_eta2p1_MET30_LooseIsoPFTau50_Trk30_eta2p1
HLT_IsoMu16_eta2p1_MET30
HLT_IsoMu17_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu17_eta2p1_LooseIsoPFTau20
HLT_IsoMu18
HLT_IsoMu19_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu19_eta2p1_LooseIsoPFTau20
HLT_IsoMu19_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu20
HLT_IsoMu21_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu21_eta2p1_LooseIsoPFTau50_Trk30_eta2p1_SingleL1
HLT_IsoMu21_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu22_eta2p1
HLT_IsoMu22
HLT_IsoMu24_eta2p1
HLT_IsoMu24
HLT_IsoMu27
HLT_IsoTkMu18
HLT_IsoTkMu20
HLT_IsoTkMu22_eta2p1
HLT_IsoTkMu22
HLT_IsoTkMu24_eta2p1
HLT_IsoTkMu24
HLT_IsoTkMu27
HLT_L1SingleMu16
HLT_L1SingleMu18
HLT_L2Mu10
HLT_Mu10_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT350_PFMETNoMu60
HLT_Mu15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Mu15_IsoVVVL_PFHT350_PFMET50
HLT_Mu15_IsoVVVL_PFHT350
HLT_Mu15_IsoVVVL_PFHT400_PFMET50
HLT_Mu15_IsoVVVL_PFHT400
HLT_Mu15_IsoVVVL_PFHT600
HLT_Mu16_eta2p1_MET30
HLT_Mu20
HLT_Mu24_eta2p1
HLT_Mu27
HLT_Mu28NoFiltersNoVtx_CentralCaloJet40
HLT_Mu28NoFiltersNoVtx_DisplacedJet40_Loose
HLT_Mu300
HLT_Mu30_eta2p1_PFJet150_PFJet50
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Loose
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Tight
HLT_Mu350
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Loose
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Tight
HLT_Mu38NoFiltersNoVtx_DisplacedJet60_Loose
HLT_Mu40_eta2p1_PFJet200_PFJet50
HLT_Mu45_eta2p1
HLT_Mu50_IsoVVVL_PFHT400
HLT_Mu50
HLT_Mu55
HLT_Mu8_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT300_PFMETNoMu60
HLT_TkMu17
HLT_TkMu20
HLT_TkMu24_eta2p1
HLT_TkMu27
HLT_TkMu50

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -8003,6 +8059,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30531/SinglePhoton_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30531/SinglePhoton_doc.html" + }, "date_created": [ "2016" ], @@ -8055,7 +8115,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-SinglePhoton-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon120_R9Id90_HE10_IsoM
HLT_Photon120
HLT_Photon135_PFMET100
HLT_Photon165_HE10
HLT_Photon165_R9Id90_HE10_IsoM
HLT_Photon175
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon22_R9Id90_HE10_IsoM
HLT_Photon22
HLT_Photon250_NoHE
HLT_Photon300_NoHE
HLT_Photon30_R9Id90_HE10_IsoM
HLT_Photon30
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon36_R9Id90_HE10_IsoM
HLT_Photon36
HLT_Photon500
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon50_R9Id90_HE10_IsoM
HLT_Photon50
HLT_Photon600
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon75_R9Id90_HE10_IsoM
HLT_Photon75
HLT_Photon90_CaloIdL_PFHT500
HLT_Photon90_CaloIdL_PFHT600
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon90_R9Id90_HE10_IsoM
HLT_Photon90

" + "description": "

Events stored in this primary dataset were selected because of the presence of one energetic photon, or one photon and high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-SinglePhoton-UL2016_MiniAODv2_NanoAODv9
Output dataset: /SinglePhoton/Run2016G-UL2016_MiniAODv2_NanoAODv9-v2/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-SinglePhoton-UL2016_MiniAODv2
Output dataset: /SinglePhoton/Run2016G-UL2016_MiniAODv2-v3/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_SinglePhoton
Output dataset: /SinglePhoton/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon120_R9Id90_HE10_IsoM
HLT_Photon120
HLT_Photon135_PFMET100
HLT_Photon165_HE10
HLT_Photon165_R9Id90_HE10_IsoM
HLT_Photon175
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon22_R9Id90_HE10_IsoM
HLT_Photon22
HLT_Photon250_NoHE
HLT_Photon300_NoHE
HLT_Photon30_R9Id90_HE10_IsoM
HLT_Photon30
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon36_R9Id90_HE10_IsoM
HLT_Photon36
HLT_Photon500
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon50_R9Id90_HE10_IsoM
HLT_Photon50
HLT_Photon600
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon75_R9Id90_HE10_IsoM
HLT_Photon75
HLT_Photon90_CaloIdL_PFHT500
HLT_Photon90_CaloIdL_PFHT600
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon90_R9Id90_HE10_IsoM
HLT_Photon90

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -8232,6 +8292,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30532/Tau_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30532/Tau_doc.html" + }, "date_created": [ "2016" ], @@ -8284,7 +8348,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-Tau-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMediumCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1
HLT_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1
HLT_IsoMu19_eta2p1_LooseCombinedIsoPFTau20
HLT_IsoMu19_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu19_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET110
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET120
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET80
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET90
HLT_LooseIsoPFTau50_Trk30_eta2p1
HLT_PFTau120_eta2p1
HLT_PFTau140_eta2p1
HLT_VLooseIsoPFTau120_Trk50_eta2p1
HLT_VLooseIsoPFTau140_Trk50_eta2p1

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one tau, or one tau and muon or high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016G-Tau-UL2016_MiniAODv2_NanoAODv9
Output dataset: /Tau/Run2016G-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016G-Tau-UL2016_MiniAODv2
Output dataset: /Tau/Run2016G-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016G_Tau
Output dataset: /Tau/Run2016G-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMediumCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1
HLT_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1
HLT_IsoMu19_eta2p1_LooseCombinedIsoPFTau20
HLT_IsoMu19_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu19_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET110
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET120
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET80
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET90
HLT_LooseIsoPFTau50_Trk30_eta2p1
HLT_PFTau120_eta2p1
HLT_PFTau140_eta2p1
HLT_VLooseIsoPFTau120_Trk50_eta2p1
HLT_VLooseIsoPFTau140_Trk50_eta2p1

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -8572,7 +8636,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-BTagCSV-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleJet90_Double30_DoubleBTagCSV_p087
HLT_DoubleJet90_Double30_TripleBTagCSV_p087
HLT_DoubleJetsC100_DoubleBTagCSV_p014_DoublePFJetsC100MaxDeta1p6
HLT_DoubleJetsC100_DoubleBTagCSV_p026_DoublePFJetsC160
HLT_DoubleJetsC100_SingleBTagCSV_p014_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p014
HLT_DoubleJetsC100_SingleBTagCSV_p026_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p026
HLT_DoubleJetsC112_DoubleBTagCSV_p014_DoublePFJetsC112MaxDeta1p6
HLT_DoubleJetsC112_DoubleBTagCSV_p026_DoublePFJetsC172
HLT_QuadJet45_DoubleBTagCSV_p087
HLT_QuadJet45_TripleBTagCSV_p087
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq460
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq500
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq200
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq240
HLT_Rsq0p02_MR300_TriPFJet80_60_40_BTagCSV_p063_p20_Mbb60_200
HLT_Rsq0p02_MR300_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR400_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR450_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR500_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR550_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two jets, tagged as b-quark jets with combined secondary vertex.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-BTagCSV-UL2016_MiniAODv2
Output dataset: /BTagCSV/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_BTagCSV
Output dataset: /BTagCSV/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleJet90_Double30_DoubleBTagCSV_p087
HLT_DoubleJet90_Double30_TripleBTagCSV_p087
HLT_DoubleJetsC100_DoubleBTagCSV_p014_DoublePFJetsC100MaxDeta1p6
HLT_DoubleJetsC100_DoubleBTagCSV_p026_DoublePFJetsC160
HLT_DoubleJetsC100_SingleBTagCSV_p014_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p014
HLT_DoubleJetsC100_SingleBTagCSV_p026_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p026
HLT_DoubleJetsC112_DoubleBTagCSV_p014_DoublePFJetsC112MaxDeta1p6
HLT_DoubleJetsC112_DoubleBTagCSV_p026_DoublePFJetsC172
HLT_QuadJet45_DoubleBTagCSV_p087
HLT_QuadJet45_TripleBTagCSV_p087
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq460
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq500
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq200
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq240
HLT_Rsq0p02_MR300_TriPFJet80_60_40_BTagCSV_p063_p20_Mbb60_200
HLT_Rsq0p02_MR300_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR400_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR450_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR500_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR550_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -8728,15 +8792,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -8856,7 +8920,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-BTagMu-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_BTagMu_AK8Jet300_Mu5
HLT_BTagMu_DiJet110_Mu5
HLT_BTagMu_DiJet170_Mu5
HLT_BTagMu_DiJet20_Mu5
HLT_BTagMu_DiJet40_Mu5
HLT_BTagMu_DiJet70_Mu5
HLT_BTagMu_Jet300_Mu5

" + "description": "

Events stored in this primary dataset were selected because of the presence of a muon from the b-quark decay, and one or more jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-BTagMu-UL2016_MiniAODv2
Output dataset: /BTagMu/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_BTagMu
Output dataset: /BTagMu/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_BTagMu_AK8Jet300_Mu5
HLT_BTagMu_DiJet110_Mu5
HLT_BTagMu_DiJet170_Mu5
HLT_BTagMu_DiJet20_Mu5
HLT_BTagMu_DiJet40_Mu5
HLT_BTagMu_DiJet70_Mu5
HLT_BTagMu_Jet300_Mu5

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -9012,15 +9076,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -9168,7 +9232,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-Charmonium-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Jpsi_Muon
HLT_Dimuon0er16_Jpsi_NoOS_NoVertexing
HLT_Dimuon0er16_Jpsi_NoVertexing
HLT_Dimuon10_Jpsi_Barrel
HLT_Dimuon13_PsiPrime
HLT_Dimuon16_Jpsi
HLT_Dimuon20_Jpsi
HLT_Dimuon6_Jpsi_NoVertexing
HLT_Dimuon8_PsiPrime_Barrel
HLT_DoubleMu4_3_Bs
HLT_DoubleMu4_3_Jpsi_Displaced
HLT_DoubleMu4_JpsiTrk_Displaced
HLT_DoubleMu4_PsiPrimeTrk_Displaced
HLT_Mu7p5_L2Mu2_Jpsi
HLT_Mu7p5_Track2_Jpsi
HLT_Mu7p5_Track3p5_Jpsi
HLT_Mu7p5_Track7_Jpsi
HLT_QuadMuon0_Dimuon0_Jpsi

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons, or a muon and a track with some requirements in the invariant mass for selecting low-mass resonances.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-Charmonium-UL2016_MiniAODv2
Output dataset: /Charmonium/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_Charmonium
Output dataset: /Charmonium/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Jpsi_Muon
HLT_Dimuon0er16_Jpsi_NoOS_NoVertexing
HLT_Dimuon0er16_Jpsi_NoVertexing
HLT_Dimuon10_Jpsi_Barrel
HLT_Dimuon13_PsiPrime
HLT_Dimuon16_Jpsi
HLT_Dimuon20_Jpsi
HLT_Dimuon6_Jpsi_NoVertexing
HLT_Dimuon8_PsiPrime_Barrel
HLT_DoubleMu4_3_Bs
HLT_DoubleMu4_3_Jpsi_Displaced
HLT_DoubleMu4_JpsiTrk_Displaced
HLT_DoubleMu4_PsiPrimeTrk_Displaced
HLT_Mu7p5_L2Mu2_Jpsi
HLT_Mu7p5_Track2_Jpsi
HLT_Mu7p5_Track3p5_Jpsi
HLT_Mu7p5_Track7_Jpsi
HLT_QuadMuon0_Dimuon0_Jpsi

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -9324,15 +9388,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -9452,7 +9516,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DisplacedJet-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_HT200_DisplacedDijet40_DisplacedTrack
HLT_HT200
HLT_HT250_DisplacedDijet40_DisplacedTrack
HLT_HT275
HLT_HT325
HLT_HT350_DisplacedDijet40_DisplacedTrack
HLT_HT350_DisplacedDijet40_Inclusive
HLT_HT350_DisplacedDijet80_DisplacedTrack
HLT_HT350_DisplacedDijet80_Tight_DisplacedTrack
HLT_HT400_DisplacedDijet40_Inclusive
HLT_HT425
HLT_HT500_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet80_Inclusive
HLT_HT575
HLT_HT650_DisplacedDijet80_Inclusive
HLT_HT750_DisplacedDijet80_Inclusive
HLT_VBF_DisplacedJet40_DisplacedTrack_2TrackIP2DSig5
HLT_VBF_DisplacedJet40_DisplacedTrack
HLT_VBF_DisplacedJet40_Hadronic_2PromptTrack
HLT_VBF_DisplacedJet40_Hadronic
HLT_VBF_DisplacedJet40_TightID_DisplacedTrack
HLT_VBF_DisplacedJet40_TightID_Hadronic
HLT_VBF_DisplacedJet40_VTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VTightID_Hadronic
HLT_VBF_DisplacedJet40_VVTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VVTightID_Hadronic

" + "description": "

Events stored in this primary dataset were selected because of the presence of one or more displaced jets, or a displaced jet and/or high scalar sum of the jet transverse momenta (HT).

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DisplacedJet-UL2016_MiniAODv2
Output dataset: /DisplacedJet/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_DisplacedJet
Output dataset: /DisplacedJet/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_HT200_DisplacedDijet40_DisplacedTrack
HLT_HT200
HLT_HT250_DisplacedDijet40_DisplacedTrack
HLT_HT275
HLT_HT325
HLT_HT350_DisplacedDijet40_DisplacedTrack
HLT_HT350_DisplacedDijet40_Inclusive
HLT_HT350_DisplacedDijet80_DisplacedTrack
HLT_HT350_DisplacedDijet80_Tight_DisplacedTrack
HLT_HT400_DisplacedDijet40_Inclusive
HLT_HT425
HLT_HT500_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet80_Inclusive
HLT_HT575
HLT_HT650_DisplacedDijet80_Inclusive
HLT_HT750_DisplacedDijet80_Inclusive
HLT_VBF_DisplacedJet40_DisplacedTrack_2TrackIP2DSig5
HLT_VBF_DisplacedJet40_DisplacedTrack
HLT_VBF_DisplacedJet40_Hadronic_2PromptTrack
HLT_VBF_DisplacedJet40_Hadronic
HLT_VBF_DisplacedJet40_TightID_DisplacedTrack
HLT_VBF_DisplacedJet40_TightID_Hadronic
HLT_VBF_DisplacedJet40_VTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VTightID_Hadronic
HLT_VBF_DisplacedJet40_VVTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VVTightID_Hadronic

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -9608,15 +9672,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -9778,7 +9842,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DoubleEG-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Diphoton30EB_18EB_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30PV_18PV_R9Id_AND_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelSeedMatch_Mass70
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_Mass90
HLT_Diphoton30_18_Solid_R9Id_AND_IsoCaloId_AND_HE_R9Id_Mass55
HLT_DoubleEle24_22_eta2p1_WPLoose_Gsf
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL_MW
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL
HLT_DoubleEle33_CaloIdL_MW
HLT_DoubleEle33_CaloIdL
HLT_DoubleEle37_Ele27_CaloIdL_GsfTrkIdVL
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_DoublePhoton60
HLT_DoublePhoton85
HLT_ECALHT800
HLT_Ele10_CaloIdM_TrackIdM_CentralPFJet30_BTagCSV_p13
HLT_Ele12_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele12_CaloIdM_TrackIdM_PFJet30
HLT_Ele16_Ele12_Ele8_CaloIdL_TrackIdL
HLT_Ele17_CaloIdL_GsfTrkIdVL
HLT_Ele17_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Ele17_CaloIdM_TrackIdM_PFJet30
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdM_TrackIdM_PFJet30
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ_L1JetTauSeeded
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele27_HighEta_Ele20_Mass55
HLT_Ele30WP60_Ele8_Mass55
HLT_Ele30WP60_SC4_Mass55
HLT_Ele8_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele8_CaloIdM_TrackIdM_PFJet30
HLT_Photon26_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon16_AND_HE10_R9Id65_Eta2_Mass60
HLT_Photon36_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon22_AND_HE10_R9Id65_Eta2_Mass15
HLT_Photon42_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon25_AND_HE10_R9Id65_Eta2_Mass15

" + "description": "

Events stored in this primary dataset were selected because of the presence of different combinations of energetic photons, electrons and/or jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DoubleEG-UL2016_MiniAODv2
Output dataset: /DoubleEG/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_DoubleEG
Output dataset: /DoubleEG/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Diphoton30EB_18EB_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30PV_18PV_R9Id_AND_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelSeedMatch_Mass70
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_Mass90
HLT_Diphoton30_18_Solid_R9Id_AND_IsoCaloId_AND_HE_R9Id_Mass55
HLT_DoubleEle24_22_eta2p1_WPLoose_Gsf
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL_MW
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL
HLT_DoubleEle33_CaloIdL_MW
HLT_DoubleEle33_CaloIdL
HLT_DoubleEle37_Ele27_CaloIdL_GsfTrkIdVL
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_DoublePhoton60
HLT_DoublePhoton85
HLT_ECALHT800
HLT_Ele10_CaloIdM_TrackIdM_CentralPFJet30_BTagCSV_p13
HLT_Ele12_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele12_CaloIdM_TrackIdM_PFJet30
HLT_Ele16_Ele12_Ele8_CaloIdL_TrackIdL
HLT_Ele17_CaloIdL_GsfTrkIdVL
HLT_Ele17_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Ele17_CaloIdM_TrackIdM_PFJet30
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdM_TrackIdM_PFJet30
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ_L1JetTauSeeded
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele27_HighEta_Ele20_Mass55
HLT_Ele30WP60_Ele8_Mass55
HLT_Ele30WP60_SC4_Mass55
HLT_Ele8_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele8_CaloIdM_TrackIdM_PFJet30
HLT_Photon26_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon16_AND_HE10_R9Id65_Eta2_Mass60
HLT_Photon36_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon22_AND_HE10_R9Id65_Eta2_Mass15
HLT_Photon42_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon25_AND_HE10_R9Id65_Eta2_Mass15

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -9935,15 +9999,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -10063,7 +10127,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DoubleMuon-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu0
HLT_DoubleMu18NoFiltersNoVtx
HLT_DoubleMu23NoFiltersNoVtxDisplaced
HLT_DoubleMu28NoFiltersNoVtxDisplaced
HLT_DoubleMu33NoFiltersNoVtx
HLT_DoubleMu38NoFiltersNoVtx
HLT_DoubleMu8_Mass8_PFHT250
HLT_DoubleMu8_Mass8_PFHT300
HLT_L2DoubleMu23_NoVertex
HLT_L2DoubleMu28_NoVertex_2Cha_Angle2p5_Mass10
HLT_L2DoubleMu38_NoVertex_2Cha_Angle2p5_Mass10
HLT_Mu10_CentralPFJet30_BTagCSV_p13
HLT_Mu17_Mu8_DZ
HLT_Mu17_Mu8_SameSign_DZ
HLT_Mu17_Mu8_SameSign
HLT_Mu17_Mu8
HLT_Mu17_TkMu8_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL
HLT_Mu17
HLT_Mu20_Mu10_DZ
HLT_Mu20_Mu10_SameSign_DZ
HLT_Mu20_Mu10_SameSign
HLT_Mu20_Mu10
HLT_Mu27_TkMu8
HLT_Mu30_TkMu11
HLT_Mu3_PFJet40
HLT_Mu40_TkMu11
HLT_Mu8_TrkIsoVVL
HLT_Mu8
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_TripleMu_12_10_5
HLT_TripleMu_5_3_3_DZ_Mass3p8
HLT_TripleMu_5_3_3
HLT_TrkMu15_DoubleTrkMu5NoFiltersNoVtx
HLT_TrkMu17_DoubleTrkMu8NoFiltersNoVtx

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two energetic muons in the event.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DoubleMuon-UL2016_MiniAODv2
Output dataset: /DoubleMuon/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_DoubleMuon
Output dataset: /DoubleMuon/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu0
HLT_DoubleMu18NoFiltersNoVtx
HLT_DoubleMu23NoFiltersNoVtxDisplaced
HLT_DoubleMu28NoFiltersNoVtxDisplaced
HLT_DoubleMu33NoFiltersNoVtx
HLT_DoubleMu38NoFiltersNoVtx
HLT_DoubleMu8_Mass8_PFHT250
HLT_DoubleMu8_Mass8_PFHT300
HLT_L2DoubleMu23_NoVertex
HLT_L2DoubleMu28_NoVertex_2Cha_Angle2p5_Mass10
HLT_L2DoubleMu38_NoVertex_2Cha_Angle2p5_Mass10
HLT_Mu10_CentralPFJet30_BTagCSV_p13
HLT_Mu17_Mu8_DZ
HLT_Mu17_Mu8_SameSign_DZ
HLT_Mu17_Mu8_SameSign
HLT_Mu17_Mu8
HLT_Mu17_TkMu8_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL
HLT_Mu17
HLT_Mu20_Mu10_DZ
HLT_Mu20_Mu10_SameSign_DZ
HLT_Mu20_Mu10_SameSign
HLT_Mu20_Mu10
HLT_Mu27_TkMu8
HLT_Mu30_TkMu11
HLT_Mu3_PFJet40
HLT_Mu40_TkMu11
HLT_Mu8_TrkIsoVVL
HLT_Mu8
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_TripleMu_12_10_5
HLT_TripleMu_5_3_3_DZ_Mass3p8
HLT_TripleMu_5_3_3
HLT_TrkMu15_DoubleTrkMu5NoFiltersNoVtx
HLT_TrkMu17_DoubleTrkMu8NoFiltersNoVtx

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -10219,15 +10283,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -10375,7 +10439,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DoubleMuonLowMass-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu3_Trk_Tau3mu
HLT_DoubleMu4_LowMassNonResonantTrk_Displaced

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons with low invariant mass.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DoubleMuonLowMass-UL2016_MiniAODv2
Output dataset: /DoubleMuonLowMass/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step ReReco-Run2016H-DoubleMuonLowMass-21Feb2020_UL2016
Output dataset: /DoubleMuonLowMass/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu3_Trk_Tau3mu
HLT_DoubleMu4_LowMassNonResonantTrk_Displaced

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -10531,15 +10595,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -10645,7 +10709,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-HTMHT-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu140
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu80
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p57
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p63
HLT_PFHT200_PFAlphaT0p51
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p55
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p58
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p54
HLT_PFHT300_PFMET100
HLT_PFHT300_PFMET110
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p52
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p51
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p52
HLT_Rsq0p25
HLT_Rsq0p30
HLT_RsqMR240_Rsq0p09_MR200_4jet
HLT_RsqMR240_Rsq0p09_MR200
HLT_RsqMR270_Rsq0p09_MR200_4jet
HLT_RsqMR270_Rsq0p09_MR200

" + "description": "

Events stored in this primary dataset were selected because of the presence of a combination of a high scalar sum of the jet transverse momenta (HT), one or more energetic jets, or high missing transverse energy.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-HTMHT-UL2016_MiniAODv2
Output dataset: /HTMHT/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_HTMHT
Output dataset: /HTMHT/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu140
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu80
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p57
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p63
HLT_PFHT200_PFAlphaT0p51
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p55
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p58
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p54
HLT_PFHT300_PFMET100
HLT_PFHT300_PFMET110
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p52
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p51
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p52
HLT_Rsq0p25
HLT_Rsq0p30
HLT_RsqMR240_Rsq0p09_MR200_4jet
HLT_RsqMR240_Rsq0p09_MR200
HLT_RsqMR270_Rsq0p09_MR200_4jet
HLT_RsqMR270_Rsq0p09_MR200

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -10801,15 +10865,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -10957,7 +11021,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-JetHT-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_AK8DiPFJet250_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet250_200_TrimMass30
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet280_200_TrimMass30
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet300_200_TrimMass30
HLT_AK8PFHT600_TrimR0p1PT0p03Mass50_BTagCSV_p20
HLT_AK8PFHT650_TrimR0p1PT0p03Mass50
HLT_AK8PFHT700_TrimR0p1PT0p03Mass50
HLT_AK8PFHT750_TrimMass50
HLT_AK8PFHT800_TrimMass50
HLT_AK8PFJet140
HLT_AK8PFJet200
HLT_AK8PFJet260
HLT_AK8PFJet320
HLT_AK8PFJet360_TrimMass30
HLT_AK8PFJet400_TrimMass30
HLT_AK8PFJet400
HLT_AK8PFJet40
HLT_AK8PFJet450
HLT_AK8PFJet500
HLT_AK8PFJet60
HLT_AK8PFJet80
HLT_CaloJet500_NoJetID
HLT_DiCentralPFJet170_CFMax0p1
HLT_DiCentralPFJet170
HLT_DiCentralPFJet220_CFMax0p3
HLT_DiCentralPFJet330_CFMax0p5
HLT_DiCentralPFJet430
HLT_DiJetVBFMu_PassThrough
HLT_DiJetVBF_PassThrough
HLT_DiPFJetAve100_HFJEC
HLT_DiPFJetAve140
HLT_DiPFJetAve160_HFJEC
HLT_DiPFJetAve200
HLT_DiPFJetAve220_HFJEC
HLT_DiPFJetAve260
HLT_DiPFJetAve300_HFJEC
HLT_DiPFJetAve320
HLT_DiPFJetAve400
HLT_DiPFJetAve40
HLT_DiPFJetAve500
HLT_DiPFJetAve60_HFJEC
HLT_DiPFJetAve60
HLT_DiPFJetAve80_HFJEC
HLT_DiPFJetAve80
HLT_HT2000
HLT_HT2500
HLT_L1_TripleJet_VBF
HLT_PFHT125
HLT_PFHT200
HLT_PFHT250
HLT_PFHT300
HLT_PFHT350
HLT_PFHT400_SixJet30_DoubleBTagCSV_p056
HLT_PFHT400_SixJet30
HLT_PFHT400
HLT_PFHT450_SixJet40_BTagCSV_p056
HLT_PFHT450_SixJet40
HLT_PFHT475
HLT_PFHT550_4JetPt50
HLT_PFHT600
HLT_PFHT650_4JetPt50
HLT_PFHT650_WideJetMJJ900DEtaJJ1p5
HLT_PFHT650_WideJetMJJ950DEtaJJ1p5
HLT_PFHT650
HLT_PFHT750_4JetPt50
HLT_PFHT750_4JetPt70
HLT_PFHT750_4JetPt80
HLT_PFHT800_4JetPt50
HLT_PFHT800
HLT_PFHT850_4JetPt50
HLT_PFHT900
HLT_PFJet140
HLT_PFJet200
HLT_PFJet260
HLT_PFJet320
HLT_PFJet400
HLT_PFJet40
HLT_PFJet450
HLT_PFJet500
HLT_PFJet60
HLT_PFJet80
HLT_QuadPFJet_VBF
HLT_SingleCentralPFJet170_CFMax0p1

" + "description": "

Events stored in this primary dataset were selected because of the presence of a high scalar sum of the jet transverse momenta (HT), or at least one or two energetic jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-JetHT-UL2016_MiniAODv2
Output dataset: /JetHT/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_JetHT
Output dataset: /JetHT/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_AK8DiPFJet250_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet250_200_TrimMass30
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet280_200_TrimMass30
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet300_200_TrimMass30
HLT_AK8PFHT600_TrimR0p1PT0p03Mass50_BTagCSV_p20
HLT_AK8PFHT650_TrimR0p1PT0p03Mass50
HLT_AK8PFHT700_TrimR0p1PT0p03Mass50
HLT_AK8PFHT750_TrimMass50
HLT_AK8PFHT800_TrimMass50
HLT_AK8PFJet140
HLT_AK8PFJet200
HLT_AK8PFJet260
HLT_AK8PFJet320
HLT_AK8PFJet360_TrimMass30
HLT_AK8PFJet400_TrimMass30
HLT_AK8PFJet400
HLT_AK8PFJet40
HLT_AK8PFJet450
HLT_AK8PFJet500
HLT_AK8PFJet60
HLT_AK8PFJet80
HLT_CaloJet500_NoJetID
HLT_DiCentralPFJet170_CFMax0p1
HLT_DiCentralPFJet170
HLT_DiCentralPFJet220_CFMax0p3
HLT_DiCentralPFJet330_CFMax0p5
HLT_DiCentralPFJet430
HLT_DiJetVBFMu_PassThrough
HLT_DiJetVBF_PassThrough
HLT_DiPFJetAve100_HFJEC
HLT_DiPFJetAve140
HLT_DiPFJetAve160_HFJEC
HLT_DiPFJetAve200
HLT_DiPFJetAve220_HFJEC
HLT_DiPFJetAve260
HLT_DiPFJetAve300_HFJEC
HLT_DiPFJetAve320
HLT_DiPFJetAve400
HLT_DiPFJetAve40
HLT_DiPFJetAve500
HLT_DiPFJetAve60_HFJEC
HLT_DiPFJetAve60
HLT_DiPFJetAve80_HFJEC
HLT_DiPFJetAve80
HLT_HT2000
HLT_HT2500
HLT_L1_TripleJet_VBF
HLT_PFHT125
HLT_PFHT200
HLT_PFHT250
HLT_PFHT300
HLT_PFHT350
HLT_PFHT400_SixJet30_DoubleBTagCSV_p056
HLT_PFHT400_SixJet30
HLT_PFHT400
HLT_PFHT450_SixJet40_BTagCSV_p056
HLT_PFHT450_SixJet40
HLT_PFHT475
HLT_PFHT550_4JetPt50
HLT_PFHT600
HLT_PFHT650_4JetPt50
HLT_PFHT650_WideJetMJJ900DEtaJJ1p5
HLT_PFHT650_WideJetMJJ950DEtaJJ1p5
HLT_PFHT650
HLT_PFHT750_4JetPt50
HLT_PFHT750_4JetPt70
HLT_PFHT750_4JetPt80
HLT_PFHT800_4JetPt50
HLT_PFHT800
HLT_PFHT850_4JetPt50
HLT_PFHT900
HLT_PFJet140
HLT_PFJet200
HLT_PFJet260
HLT_PFJet320
HLT_PFJet400
HLT_PFJet40
HLT_PFJet450
HLT_PFJet500
HLT_PFJet60
HLT_PFJet80
HLT_QuadPFJet_VBF
HLT_SingleCentralPFJet170_CFMax0p1

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -11113,15 +11177,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -11241,7 +11305,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-MET-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight_BTagCSV_p067
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight
HLT_DiCentralPFJet55_PFMET110
HLT_DoubleMu3_PFMET50
HLT_MET200
HLT_MET250
HLT_MET300
HLT_MET600
HLT_MET60_IsoTrk35_Loose
HLT_MET700
HLT_MET75_IsoTrk50
HLT_MET90_IsoTrk50
HLT_MonoCentralPFJet80_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_Mu14er_PFMET100
HLT_Mu3er_PFHT140_PFMET125
HLT_Mu6_PFHT200_PFMET100
HLT_Mu6_PFHT200_PFMET80_BTagCSV_p067
HLT_PFMET100_PFMHT100_IDTight_BeamHaloCleaned
HLT_PFMET100_PFMHT100_IDTight
HLT_PFMET110_PFMHT110_IDTight
HLT_PFMET120_BTagCSV_p067
HLT_PFMET120_Mu5
HLT_PFMET120_PFMHT120_IDTight
HLT_PFMET170_BeamHaloCleaned
HLT_PFMET170_HBHECleaned
HLT_PFMET170_HBHE_BeamHaloCleaned
HLT_PFMET170_JetIdCleaned
HLT_PFMET170_NoiseCleaned
HLT_PFMET170_NotCleaned
HLT_PFMET300
HLT_PFMET400
HLT_PFMET500
HLT_PFMET600
HLT_PFMET90_PFMHT90_IDTight
HLT_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_PFMETTypeOne190_HBHE_BeamHaloCleaned

" + "description": "

Events stored in this primary dataset were selected because of the presence of high missing transverse energy.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-MET-UL2016_MiniAODv2
Output dataset: /MET/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_MET
Output dataset: /MET/Run2016H-21Feb2020_UL2016-v2/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight_BTagCSV_p067
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight
HLT_DiCentralPFJet55_PFMET110
HLT_DoubleMu3_PFMET50
HLT_MET200
HLT_MET250
HLT_MET300
HLT_MET600
HLT_MET60_IsoTrk35_Loose
HLT_MET700
HLT_MET75_IsoTrk50
HLT_MET90_IsoTrk50
HLT_MonoCentralPFJet80_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_Mu14er_PFMET100
HLT_Mu3er_PFHT140_PFMET125
HLT_Mu6_PFHT200_PFMET100
HLT_Mu6_PFHT200_PFMET80_BTagCSV_p067
HLT_PFMET100_PFMHT100_IDTight_BeamHaloCleaned
HLT_PFMET100_PFMHT100_IDTight
HLT_PFMET110_PFMHT110_IDTight
HLT_PFMET120_BTagCSV_p067
HLT_PFMET120_Mu5
HLT_PFMET120_PFMHT120_IDTight
HLT_PFMET170_BeamHaloCleaned
HLT_PFMET170_HBHECleaned
HLT_PFMET170_HBHE_BeamHaloCleaned
HLT_PFMET170_JetIdCleaned
HLT_PFMET170_NoiseCleaned
HLT_PFMET170_NotCleaned
HLT_PFMET300
HLT_PFMET400
HLT_PFMET500
HLT_PFMET600
HLT_PFMET90_PFMHT90_IDTight
HLT_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_PFMETTypeOne190_HBHE_BeamHaloCleaned

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -11397,15 +11461,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -11539,7 +11603,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-MuOnia-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Phi_Barrel
HLT_Dimuon0_Upsilon_Muon
HLT_Dimuon13_Upsilon
HLT_Dimuon8_Upsilon_Barrel
HLT_Mu16_TkMu0_dEta18_Onia
HLT_Mu16_TkMu0_dEta18_Phi
HLT_Mu25_TkMu0_dEta18_Onia
HLT_Mu7p5_L2Mu2_Upsilon
HLT_Mu7p5_Track2_Upsilon
HLT_Mu7p5_Track3p5_Upsilon
HLT_Mu7p5_Track7_Upsilon
HLT_QuadMuon0_Dimuon0_Upsilon

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons in the event requiring only very low energy and some requirements in the invariant mass for selecting low-mass resonances.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-MuOnia-UL2016_MiniAODv2
Output dataset: /MuOnia/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_MuOnia
Output dataset: /MuOnia/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Phi_Barrel
HLT_Dimuon0_Upsilon_Muon
HLT_Dimuon13_Upsilon
HLT_Dimuon8_Upsilon_Barrel
HLT_Mu16_TkMu0_dEta18_Onia
HLT_Mu16_TkMu0_dEta18_Phi
HLT_Mu25_TkMu0_dEta18_Onia
HLT_Mu7p5_L2Mu2_Upsilon
HLT_Mu7p5_Track2_Upsilon
HLT_Mu7p5_Track3p5_Upsilon
HLT_Mu7p5_Track7_Upsilon
HLT_QuadMuon0_Dimuon0_Upsilon

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -11695,15 +11759,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -11809,7 +11873,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-MuonEG-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiMu9_Ele9_CaloIdL_TrackIdL
HLT_Mu12_Photon25_CaloIdL_L1ISO
HLT_Mu12_Photon25_CaloIdL_L1OR
HLT_Mu12_Photon25_CaloIdL
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Mu17_Photon22_CaloIdL_L1ISO
HLT_Mu17_Photon30_CaloIdL_L1ISO
HLT_Mu17_Photon35_CaloIdL_L1ISO
HLT_Mu17_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23NoFiltersNoVtx_Photon23_CaloIdL
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL
HLT_Mu27_Ele37_CaloIdL_GsfTrkIdVL
HLT_Mu28NoFiltersNoVtxDisplaced_Photon28_CaloIdL
HLT_Mu30_Ele30_CaloIdL_GsfTrkIdVL
HLT_Mu33NoFiltersNoVtxDisplaced_Photon33_CaloIdL
HLT_Mu33_Ele33_CaloIdL_GsfTrkIdVL
HLT_Mu37_Ele27_CaloIdL_GsfTrkIdVL
HLT_Mu38NoFiltersNoVtx_Photon38_CaloIdL
HLT_Mu42NoFiltersNoVtx_Photon42_CaloIdL
HLT_Mu8_DiEle12_CaloIdL_TrackIdL
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_Mu8_TrkIsoVVL_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL

" + "description": "

Events stored in this primary dataset were selected because of the presence of one energetic muon and electron or photon.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-MuonEG-UL2016_MiniAODv2
Output dataset: /MuonEG/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_MuonEG
Output dataset: /MuonEG/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiMu9_Ele9_CaloIdL_TrackIdL
HLT_Mu12_Photon25_CaloIdL_L1ISO
HLT_Mu12_Photon25_CaloIdL_L1OR
HLT_Mu12_Photon25_CaloIdL
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Mu17_Photon22_CaloIdL_L1ISO
HLT_Mu17_Photon30_CaloIdL_L1ISO
HLT_Mu17_Photon35_CaloIdL_L1ISO
HLT_Mu17_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23NoFiltersNoVtx_Photon23_CaloIdL
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL
HLT_Mu27_Ele37_CaloIdL_GsfTrkIdVL
HLT_Mu28NoFiltersNoVtxDisplaced_Photon28_CaloIdL
HLT_Mu30_Ele30_CaloIdL_GsfTrkIdVL
HLT_Mu33NoFiltersNoVtxDisplaced_Photon33_CaloIdL
HLT_Mu33_Ele33_CaloIdL_GsfTrkIdVL
HLT_Mu37_Ele27_CaloIdL_GsfTrkIdVL
HLT_Mu38NoFiltersNoVtx_Photon38_CaloIdL
HLT_Mu42NoFiltersNoVtx_Photon42_CaloIdL
HLT_Mu8_DiEle12_CaloIdL_TrackIdL
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_Mu8_TrkIsoVVL_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -11965,15 +12029,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -12121,7 +12185,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Ele105_CaloIdVT_GsfTrkIdT
HLT_Ele115_CaloIdVT_GsfTrkIdT
HLT_Ele145_CaloIdVT_GsfTrkIdT
HLT_Ele15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Ele15_IsoVVVL_PFHT350_PFMET50
HLT_Ele15_IsoVVVL_PFHT350
HLT_Ele15_IsoVVVL_PFHT400_PFMET50
HLT_Ele15_IsoVVVL_PFHT400
HLT_Ele15_IsoVVVL_PFHT600
HLT_Ele200_CaloIdVT_GsfTrkIdT
HLT_Ele20_eta2p1_WPLoose_Gsf_LooseIsoPFTau28
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau29
HLT_Ele22_eta2p1_WPLoose_Gsf
HLT_Ele23_WPLoose_Gsf_WHbbBoost
HLT_Ele23_WPLoose_Gsf
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau30
HLT_Ele24_eta2p1_WPLoose_Gsf
HLT_Ele250_CaloIdVT_GsfTrkIdT
HLT_Ele25_WPTight_Gsf
HLT_Ele25_eta2p1_WPLoose_Gsf
HLT_Ele25_eta2p1_WPTight_Gsf
HLT_Ele27_WPLoose_Gsf_WHbbBoost
HLT_Ele27_WPLoose_Gsf
HLT_Ele27_WPTight_Gsf_L1JetTauSeeded
HLT_Ele27_WPTight_Gsf
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_HT200
HLT_Ele27_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele27_eta2p1_WPLoose_Gsf
HLT_Ele27_eta2p1_WPTight_Gsf
HLT_Ele300_CaloIdVT_GsfTrkIdT
HLT_Ele30_WPTight_Gsf
HLT_Ele30_eta2p1_WPTight_Gsf
HLT_Ele32_WPTight_Gsf
HLT_Ele32_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele32_eta2p1_WPTight_Gsf
HLT_Ele35_CaloIdVT_GsfTrkIdT_PFJet150_PFJet50
HLT_Ele35_WPLoose_Gsf
HLT_Ele36_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele45_CaloIdVT_GsfTrkIdT_PFJet200_PFJet50
HLT_Ele45_WPLoose_Gsf_L1JetTauSeeded
HLT_Ele45_WPLoose_Gsf
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet140
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet165
HLT_Ele50_IsoVVVL_PFHT400

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one high-energy electron, or at least one high-energy electron and one or more jets or tau.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2
Output dataset: /SingleElectron/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_SingleElectron
Output dataset: /SingleElectron/Run2016H-21Feb2020_UL2016-v2/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Ele105_CaloIdVT_GsfTrkIdT
HLT_Ele115_CaloIdVT_GsfTrkIdT
HLT_Ele145_CaloIdVT_GsfTrkIdT
HLT_Ele15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Ele15_IsoVVVL_PFHT350_PFMET50
HLT_Ele15_IsoVVVL_PFHT350
HLT_Ele15_IsoVVVL_PFHT400_PFMET50
HLT_Ele15_IsoVVVL_PFHT400
HLT_Ele15_IsoVVVL_PFHT600
HLT_Ele200_CaloIdVT_GsfTrkIdT
HLT_Ele20_eta2p1_WPLoose_Gsf_LooseIsoPFTau28
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau29
HLT_Ele22_eta2p1_WPLoose_Gsf
HLT_Ele23_WPLoose_Gsf_WHbbBoost
HLT_Ele23_WPLoose_Gsf
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau30
HLT_Ele24_eta2p1_WPLoose_Gsf
HLT_Ele250_CaloIdVT_GsfTrkIdT
HLT_Ele25_WPTight_Gsf
HLT_Ele25_eta2p1_WPLoose_Gsf
HLT_Ele25_eta2p1_WPTight_Gsf
HLT_Ele27_WPLoose_Gsf_WHbbBoost
HLT_Ele27_WPLoose_Gsf
HLT_Ele27_WPTight_Gsf_L1JetTauSeeded
HLT_Ele27_WPTight_Gsf
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_HT200
HLT_Ele27_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele27_eta2p1_WPLoose_Gsf
HLT_Ele27_eta2p1_WPTight_Gsf
HLT_Ele300_CaloIdVT_GsfTrkIdT
HLT_Ele30_WPTight_Gsf
HLT_Ele30_eta2p1_WPTight_Gsf
HLT_Ele32_WPTight_Gsf
HLT_Ele32_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele32_eta2p1_WPTight_Gsf
HLT_Ele35_CaloIdVT_GsfTrkIdT_PFJet150_PFJet50
HLT_Ele35_WPLoose_Gsf
HLT_Ele36_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele45_CaloIdVT_GsfTrkIdT_PFJet200_PFJet50
HLT_Ele45_WPLoose_Gsf_L1JetTauSeeded
HLT_Ele45_WPLoose_Gsf
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet140
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet165
HLT_Ele50_IsoVVVL_PFHT400

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -12278,15 +12342,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -12434,7 +12498,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-SingleMuon-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleIsoMu17_eta2p1_noDzCut
HLT_DoubleIsoMu17_eta2p1
HLT_IsoMu16_eta2p1_MET30_LooseIsoPFTau50_Trk30_eta2p1
HLT_IsoMu16_eta2p1_MET30
HLT_IsoMu17_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu17_eta2p1_LooseIsoPFTau20
HLT_IsoMu18
HLT_IsoMu19_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu19_eta2p1_LooseIsoPFTau20
HLT_IsoMu19_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu20
HLT_IsoMu21_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu21_eta2p1_LooseIsoPFTau50_Trk30_eta2p1_SingleL1
HLT_IsoMu21_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu22_eta2p1
HLT_IsoMu22
HLT_IsoMu24_eta2p1
HLT_IsoMu24
HLT_IsoMu27
HLT_IsoTkMu18
HLT_IsoTkMu20
HLT_IsoTkMu22_eta2p1
HLT_IsoTkMu22
HLT_IsoTkMu24_eta2p1
HLT_IsoTkMu24
HLT_IsoTkMu27
HLT_L1SingleMu16
HLT_L1SingleMu18
HLT_L2Mu10
HLT_Mu10_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT350_PFMETNoMu60
HLT_Mu15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Mu15_IsoVVVL_PFHT350_PFMET50
HLT_Mu15_IsoVVVL_PFHT350
HLT_Mu15_IsoVVVL_PFHT400_PFMET50
HLT_Mu15_IsoVVVL_PFHT400
HLT_Mu15_IsoVVVL_PFHT600
HLT_Mu16_eta2p1_MET30
HLT_Mu20
HLT_Mu24_eta2p1
HLT_Mu27
HLT_Mu28NoFiltersNoVtx_CentralCaloJet40
HLT_Mu28NoFiltersNoVtx_DisplacedJet40_Loose
HLT_Mu300
HLT_Mu30_eta2p1_PFJet150_PFJet50
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Loose
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Tight
HLT_Mu350
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Loose
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Tight
HLT_Mu38NoFiltersNoVtx_DisplacedJet60_Loose
HLT_Mu40_eta2p1_PFJet200_PFJet50
HLT_Mu45_eta2p1
HLT_Mu50_IsoVVVL_PFHT400
HLT_Mu50
HLT_Mu55
HLT_Mu8_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT300_PFMETNoMu60
HLT_TkMu17
HLT_TkMu20
HLT_TkMu24_eta2p1
HLT_TkMu27
HLT_TkMu50

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one energetic muon, or at least one muon and one or more jets, tau or high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-SingleMuon-UL2016_MiniAODv2
Output dataset: /SingleMuon/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_SingleMuon
Output dataset: /SingleMuon/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleIsoMu17_eta2p1_noDzCut
HLT_DoubleIsoMu17_eta2p1
HLT_IsoMu16_eta2p1_MET30_LooseIsoPFTau50_Trk30_eta2p1
HLT_IsoMu16_eta2p1_MET30
HLT_IsoMu17_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu17_eta2p1_LooseIsoPFTau20
HLT_IsoMu18
HLT_IsoMu19_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu19_eta2p1_LooseIsoPFTau20
HLT_IsoMu19_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu20
HLT_IsoMu21_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu21_eta2p1_LooseIsoPFTau50_Trk30_eta2p1_SingleL1
HLT_IsoMu21_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu22_eta2p1
HLT_IsoMu22
HLT_IsoMu24_eta2p1
HLT_IsoMu24
HLT_IsoMu27
HLT_IsoTkMu18
HLT_IsoTkMu20
HLT_IsoTkMu22_eta2p1
HLT_IsoTkMu22
HLT_IsoTkMu24_eta2p1
HLT_IsoTkMu24
HLT_IsoTkMu27
HLT_L1SingleMu16
HLT_L1SingleMu18
HLT_L2Mu10
HLT_Mu10_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT350_PFMETNoMu60
HLT_Mu15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Mu15_IsoVVVL_PFHT350_PFMET50
HLT_Mu15_IsoVVVL_PFHT350
HLT_Mu15_IsoVVVL_PFHT400_PFMET50
HLT_Mu15_IsoVVVL_PFHT400
HLT_Mu15_IsoVVVL_PFHT600
HLT_Mu16_eta2p1_MET30
HLT_Mu20
HLT_Mu24_eta2p1
HLT_Mu27
HLT_Mu28NoFiltersNoVtx_CentralCaloJet40
HLT_Mu28NoFiltersNoVtx_DisplacedJet40_Loose
HLT_Mu300
HLT_Mu30_eta2p1_PFJet150_PFJet50
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Loose
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Tight
HLT_Mu350
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Loose
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Tight
HLT_Mu38NoFiltersNoVtx_DisplacedJet60_Loose
HLT_Mu40_eta2p1_PFJet200_PFJet50
HLT_Mu45_eta2p1
HLT_Mu50_IsoVVVL_PFHT400
HLT_Mu50
HLT_Mu55
HLT_Mu8_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT300_PFMETNoMu60
HLT_TkMu17
HLT_TkMu20
HLT_TkMu24_eta2p1
HLT_TkMu27
HLT_TkMu50

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -12590,15 +12654,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -12718,7 +12782,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-SinglePhoton-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon120_R9Id90_HE10_IsoM
HLT_Photon120
HLT_Photon135_PFMET100
HLT_Photon165_HE10
HLT_Photon165_R9Id90_HE10_IsoM
HLT_Photon175
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon22_R9Id90_HE10_IsoM
HLT_Photon22
HLT_Photon250_NoHE
HLT_Photon300_NoHE
HLT_Photon30_R9Id90_HE10_IsoM
HLT_Photon30
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon36_R9Id90_HE10_IsoM
HLT_Photon36
HLT_Photon500
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon50_R9Id90_HE10_IsoM
HLT_Photon50
HLT_Photon600
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon75_R9Id90_HE10_IsoM
HLT_Photon75
HLT_Photon90_CaloIdL_PFHT500
HLT_Photon90_CaloIdL_PFHT600
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon90_R9Id90_HE10_IsoM
HLT_Photon90

" + "description": "

Events stored in this primary dataset were selected because of the presence of one energetic photon, or one photon and high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-SinglePhoton-UL2016_MiniAODv2
Output dataset: /SinglePhoton/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_SinglePhoton
Output dataset: /SinglePhoton/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon120_R9Id90_HE10_IsoM
HLT_Photon120
HLT_Photon135_PFMET100
HLT_Photon165_HE10
HLT_Photon165_R9Id90_HE10_IsoM
HLT_Photon175
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon22_R9Id90_HE10_IsoM
HLT_Photon22
HLT_Photon250_NoHE
HLT_Photon300_NoHE
HLT_Photon30_R9Id90_HE10_IsoM
HLT_Photon30
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon36_R9Id90_HE10_IsoM
HLT_Photon36
HLT_Photon500
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon50_R9Id90_HE10_IsoM
HLT_Photon50
HLT_Photon600
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon75_R9Id90_HE10_IsoM
HLT_Photon75
HLT_Photon90_CaloIdL_PFHT500
HLT_Photon90_CaloIdL_PFHT600
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon90_R9Id90_HE10_IsoM
HLT_Photon90

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -12875,15 +12939,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -13031,7 +13095,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-Tau-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMediumCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1
HLT_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1
HLT_IsoMu19_eta2p1_LooseCombinedIsoPFTau20
HLT_IsoMu19_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu19_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET110
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET120
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET80
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET90
HLT_LooseIsoPFTau50_Trk30_eta2p1
HLT_PFTau120_eta2p1
HLT_PFTau140_eta2p1
HLT_VLooseIsoPFTau120_Trk50_eta2p1
HLT_VLooseIsoPFTau140_Trk50_eta2p1

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one tau, or one tau and muon or high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-Tau-UL2016_MiniAODv2
Output dataset: /Tau/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_Tau
Output dataset: /Tau/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMediumCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1
HLT_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1
HLT_IsoMu19_eta2p1_LooseCombinedIsoPFTau20
HLT_IsoMu19_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu19_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET110
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET120
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET80
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET90
HLT_LooseIsoPFTau50_Trk30_eta2p1
HLT_PFTau120_eta2p1
HLT_PFTau140_eta2p1
HLT_VLooseIsoPFTau120_Trk50_eta2p1
HLT_VLooseIsoPFTau140_Trk50_eta2p1

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -13187,15 +13251,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -13315,7 +13379,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / PAT
This primary MINIAOD dataset was processed from the RAW dataset by the following step:
Step: PAT
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-ZeroBias-UL2016_MiniAODv2\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Random

" + "description": "

This primary dataset is an unbiased sample of all collisions.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This MINIAOD dataset was processed from the RAW dataset by the following steps:

Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-ZeroBias-UL2016_MiniAODv2
Output dataset: /ZeroBias/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_ZeroBias
Output dataset: /ZeroBias/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Random

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -13464,15 +13528,15 @@ "links": [ { "description": "Running CMS analysis code using Docker", - "url": "/docs/cms-guide-docker" + "url": "/docs/cms-guide-docker#images" }, { "description": "How to install the CMS Virtual Machine", - "url": "/docs/cms-virtual-machine-2016-2018" + "url": "/docs/cms-virtual-machine-cc7" }, { "description": "Getting started with CMS open data", - "url": "/docs/cms-getting-started-2016-2018" + "url": "/docs/cms-getting-started-miniaod" } ] }, @@ -13512,6 +13576,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30550/BTagCSV_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30550/BTagCSV_doc.html" + }, "date_created": [ "2016" ], @@ -13550,7 +13618,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-BTagCSV-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleJet90_Double30_DoubleBTagCSV_p087
HLT_DoubleJet90_Double30_TripleBTagCSV_p087
HLT_DoubleJetsC100_DoubleBTagCSV_p014_DoublePFJetsC100MaxDeta1p6
HLT_DoubleJetsC100_DoubleBTagCSV_p026_DoublePFJetsC160
HLT_DoubleJetsC100_SingleBTagCSV_p014_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p014
HLT_DoubleJetsC100_SingleBTagCSV_p026_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p026
HLT_DoubleJetsC112_DoubleBTagCSV_p014_DoublePFJetsC112MaxDeta1p6
HLT_DoubleJetsC112_DoubleBTagCSV_p026_DoublePFJetsC172
HLT_QuadJet45_DoubleBTagCSV_p087
HLT_QuadJet45_TripleBTagCSV_p087
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq460
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq500
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq200
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq240
HLT_Rsq0p02_MR300_TriPFJet80_60_40_BTagCSV_p063_p20_Mbb60_200
HLT_Rsq0p02_MR300_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR400_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR450_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR500_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR550_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two jets, tagged as b-quark jets with combined secondary vertex.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-BTagCSV-UL2016_MiniAODv2_NanoAODv9
Output dataset: /BTagCSV/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-BTagCSV-UL2016_MiniAODv2
Output dataset: /BTagCSV/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_BTagCSV
Output dataset: /BTagCSV/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleJet90_Double30_DoubleBTagCSV_p087
HLT_DoubleJet90_Double30_TripleBTagCSV_p087
HLT_DoubleJetsC100_DoubleBTagCSV_p014_DoublePFJetsC100MaxDeta1p6
HLT_DoubleJetsC100_DoubleBTagCSV_p026_DoublePFJetsC160
HLT_DoubleJetsC100_SingleBTagCSV_p014_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p014
HLT_DoubleJetsC100_SingleBTagCSV_p026_SinglePFJetC350
HLT_DoubleJetsC100_SingleBTagCSV_p026
HLT_DoubleJetsC112_DoubleBTagCSV_p014_DoublePFJetsC112MaxDeta1p6
HLT_DoubleJetsC112_DoubleBTagCSV_p026_DoublePFJetsC172
HLT_QuadJet45_DoubleBTagCSV_p087
HLT_QuadJet45_TripleBTagCSV_p087
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq460
HLT_QuadPFJet_BTagCSV_p016_VBF_Mqq500
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq200
HLT_QuadPFJet_BTagCSV_p016_p11_VBF_Mqq240
HLT_Rsq0p02_MR300_TriPFJet80_60_40_BTagCSV_p063_p20_Mbb60_200
HLT_Rsq0p02_MR300_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR400_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR450_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR500_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200
HLT_Rsq0p02_MR550_TriPFJet80_60_40_DoubleBTagCSV_p063_Mbb60_200

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -13749,6 +13817,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30551/BTagMu_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30551/BTagMu_doc.html" + }, "date_created": [ "2016" ], @@ -13787,7 +13859,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-BTagMu-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_BTagMu_AK8Jet300_Mu5
HLT_BTagMu_DiJet110_Mu5
HLT_BTagMu_DiJet170_Mu5
HLT_BTagMu_DiJet20_Mu5
HLT_BTagMu_DiJet40_Mu5
HLT_BTagMu_DiJet70_Mu5
HLT_BTagMu_Jet300_Mu5

" + "description": "

Events stored in this primary dataset were selected because of the presence of a muon from the b-quark decay, and one or more jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-BTagMu-UL2016_MiniAODv2_NanoAODv9
Output dataset: /BTagMu/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-BTagMu-UL2016_MiniAODv2
Output dataset: /BTagMu/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_BTagMu
Output dataset: /BTagMu/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_BTagMu_AK8Jet300_Mu5
HLT_BTagMu_DiJet110_Mu5
HLT_BTagMu_DiJet170_Mu5
HLT_BTagMu_DiJet20_Mu5
HLT_BTagMu_DiJet40_Mu5
HLT_BTagMu_DiJet70_Mu5
HLT_BTagMu_Jet300_Mu5

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -13986,6 +14058,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30552/Charmonium_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30552/Charmonium_doc.html" + }, "date_created": [ "2016" ], @@ -14024,7 +14100,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-Charmonium-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Jpsi_Muon
HLT_Dimuon0er16_Jpsi_NoOS_NoVertexing
HLT_Dimuon0er16_Jpsi_NoVertexing
HLT_Dimuon10_Jpsi_Barrel
HLT_Dimuon13_PsiPrime
HLT_Dimuon16_Jpsi
HLT_Dimuon20_Jpsi
HLT_Dimuon6_Jpsi_NoVertexing
HLT_Dimuon8_PsiPrime_Barrel
HLT_DoubleMu4_3_Bs
HLT_DoubleMu4_3_Jpsi_Displaced
HLT_DoubleMu4_JpsiTrk_Displaced
HLT_DoubleMu4_PsiPrimeTrk_Displaced
HLT_Mu7p5_L2Mu2_Jpsi
HLT_Mu7p5_Track2_Jpsi
HLT_Mu7p5_Track3p5_Jpsi
HLT_Mu7p5_Track7_Jpsi
HLT_QuadMuon0_Dimuon0_Jpsi

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons, or a muon and a track with some requirements in the invariant mass for selecting low-mass resonances.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-Charmonium-UL2016_MiniAODv2_NanoAODv9
Output dataset: /Charmonium/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-Charmonium-UL2016_MiniAODv2
Output dataset: /Charmonium/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_Charmonium
Output dataset: /Charmonium/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Jpsi_Muon
HLT_Dimuon0er16_Jpsi_NoOS_NoVertexing
HLT_Dimuon0er16_Jpsi_NoVertexing
HLT_Dimuon10_Jpsi_Barrel
HLT_Dimuon13_PsiPrime
HLT_Dimuon16_Jpsi
HLT_Dimuon20_Jpsi
HLT_Dimuon6_Jpsi_NoVertexing
HLT_Dimuon8_PsiPrime_Barrel
HLT_DoubleMu4_3_Bs
HLT_DoubleMu4_3_Jpsi_Displaced
HLT_DoubleMu4_JpsiTrk_Displaced
HLT_DoubleMu4_PsiPrimeTrk_Displaced
HLT_Mu7p5_L2Mu2_Jpsi
HLT_Mu7p5_Track2_Jpsi
HLT_Mu7p5_Track3p5_Jpsi
HLT_Mu7p5_Track7_Jpsi
HLT_QuadMuon0_Dimuon0_Jpsi

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -14223,6 +14299,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30553/DisplacedJet_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30553/DisplacedJet_doc.html" + }, "date_created": [ "2016" ], @@ -14261,7 +14341,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-DisplacedJet-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_HT200_DisplacedDijet40_DisplacedTrack
HLT_HT200
HLT_HT250_DisplacedDijet40_DisplacedTrack
HLT_HT275
HLT_HT325
HLT_HT350_DisplacedDijet40_DisplacedTrack
HLT_HT350_DisplacedDijet40_Inclusive
HLT_HT350_DisplacedDijet80_DisplacedTrack
HLT_HT350_DisplacedDijet80_Tight_DisplacedTrack
HLT_HT400_DisplacedDijet40_Inclusive
HLT_HT425
HLT_HT500_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet80_Inclusive
HLT_HT575
HLT_HT650_DisplacedDijet80_Inclusive
HLT_HT750_DisplacedDijet80_Inclusive
HLT_VBF_DisplacedJet40_DisplacedTrack_2TrackIP2DSig5
HLT_VBF_DisplacedJet40_DisplacedTrack
HLT_VBF_DisplacedJet40_Hadronic_2PromptTrack
HLT_VBF_DisplacedJet40_Hadronic
HLT_VBF_DisplacedJet40_TightID_DisplacedTrack
HLT_VBF_DisplacedJet40_TightID_Hadronic
HLT_VBF_DisplacedJet40_VTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VTightID_Hadronic
HLT_VBF_DisplacedJet40_VVTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VVTightID_Hadronic

" + "description": "

Events stored in this primary dataset were selected because of the presence of one or more displaced jets, or a displaced jet and/or high scalar sum of the jet transverse momenta (HT).

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-DisplacedJet-UL2016_MiniAODv2_NanoAODv9
Output dataset: /DisplacedJet/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DisplacedJet-UL2016_MiniAODv2
Output dataset: /DisplacedJet/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_DisplacedJet
Output dataset: /DisplacedJet/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_HT200_DisplacedDijet40_DisplacedTrack
HLT_HT200
HLT_HT250_DisplacedDijet40_DisplacedTrack
HLT_HT275
HLT_HT325
HLT_HT350_DisplacedDijet40_DisplacedTrack
HLT_HT350_DisplacedDijet40_Inclusive
HLT_HT350_DisplacedDijet80_DisplacedTrack
HLT_HT350_DisplacedDijet80_Tight_DisplacedTrack
HLT_HT400_DisplacedDijet40_Inclusive
HLT_HT425
HLT_HT500_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet40_Inclusive
HLT_HT550_DisplacedDijet80_Inclusive
HLT_HT575
HLT_HT650_DisplacedDijet80_Inclusive
HLT_HT750_DisplacedDijet80_Inclusive
HLT_VBF_DisplacedJet40_DisplacedTrack_2TrackIP2DSig5
HLT_VBF_DisplacedJet40_DisplacedTrack
HLT_VBF_DisplacedJet40_Hadronic_2PromptTrack
HLT_VBF_DisplacedJet40_Hadronic
HLT_VBF_DisplacedJet40_TightID_DisplacedTrack
HLT_VBF_DisplacedJet40_TightID_Hadronic
HLT_VBF_DisplacedJet40_VTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VTightID_Hadronic
HLT_VBF_DisplacedJet40_VVTightID_DisplacedTrack
HLT_VBF_DisplacedJet40_VVTightID_Hadronic

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -14460,6 +14540,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30554/DoubleEG_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30554/DoubleEG_doc.html" + }, "date_created": [ "2016" ], @@ -14526,7 +14610,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-DoubleEG-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Diphoton30EB_18EB_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30PV_18PV_R9Id_AND_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelSeedMatch_Mass70
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_Mass90
HLT_Diphoton30_18_Solid_R9Id_AND_IsoCaloId_AND_HE_R9Id_Mass55
HLT_DoubleEle24_22_eta2p1_WPLoose_Gsf
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL_MW
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL
HLT_DoubleEle33_CaloIdL_MW
HLT_DoubleEle33_CaloIdL
HLT_DoubleEle37_Ele27_CaloIdL_GsfTrkIdVL
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_DoublePhoton60
HLT_DoublePhoton85
HLT_ECALHT800
HLT_Ele10_CaloIdM_TrackIdM_CentralPFJet30_BTagCSV_p13
HLT_Ele12_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele12_CaloIdM_TrackIdM_PFJet30
HLT_Ele16_Ele12_Ele8_CaloIdL_TrackIdL
HLT_Ele17_CaloIdL_GsfTrkIdVL
HLT_Ele17_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Ele17_CaloIdM_TrackIdM_PFJet30
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdM_TrackIdM_PFJet30
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ_L1JetTauSeeded
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele27_HighEta_Ele20_Mass55
HLT_Ele30WP60_Ele8_Mass55
HLT_Ele30WP60_SC4_Mass55
HLT_Ele8_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele8_CaloIdM_TrackIdM_PFJet30
HLT_Photon26_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon16_AND_HE10_R9Id65_Eta2_Mass60
HLT_Photon36_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon22_AND_HE10_R9Id65_Eta2_Mass15
HLT_Photon42_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon25_AND_HE10_R9Id65_Eta2_Mass15

" + "description": "

Events stored in this primary dataset were selected because of the presence of different combinations of energetic photons, electrons and/or jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-DoubleEG-UL2016_MiniAODv2_NanoAODv9
Output dataset: /DoubleEG/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DoubleEG-UL2016_MiniAODv2
Output dataset: /DoubleEG/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_DoubleEG
Output dataset: /DoubleEG/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Diphoton30EB_18EB_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30PV_18PV_R9Id_AND_IsoCaloId_AND_HE_R9Id_DoublePixelVeto_Mass55
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_DoublePixelSeedMatch_Mass70
HLT_Diphoton30_18_R9Id_OR_IsoCaloId_AND_HE_R9Id_Mass90
HLT_Diphoton30_18_Solid_R9Id_AND_IsoCaloId_AND_HE_R9Id_Mass55
HLT_DoubleEle24_22_eta2p1_WPLoose_Gsf
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL_MW
HLT_DoubleEle33_CaloIdL_GsfTrkIdVL
HLT_DoubleEle33_CaloIdL_MW
HLT_DoubleEle33_CaloIdL
HLT_DoubleEle37_Ele27_CaloIdL_GsfTrkIdVL
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_DoubleEle8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_DoublePhoton60
HLT_DoublePhoton85
HLT_ECALHT800
HLT_Ele10_CaloIdM_TrackIdM_CentralPFJet30_BTagCSV_p13
HLT_Ele12_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele12_CaloIdM_TrackIdM_PFJet30
HLT_Ele16_Ele12_Ele8_CaloIdL_TrackIdL
HLT_Ele17_CaloIdL_GsfTrkIdVL
HLT_Ele17_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Ele17_CaloIdM_TrackIdM_PFJet30
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele17_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Ele23_CaloIdM_TrackIdM_PFJet30
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ_L1JetTauSeeded
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Ele23_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Ele27_HighEta_Ele20_Mass55
HLT_Ele30WP60_Ele8_Mass55
HLT_Ele30WP60_SC4_Mass55
HLT_Ele8_CaloIdL_TrackIdL_IsoVL_PFJet30
HLT_Ele8_CaloIdM_TrackIdM_PFJet30
HLT_Photon26_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon16_AND_HE10_R9Id65_Eta2_Mass60
HLT_Photon36_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon22_AND_HE10_R9Id65_Eta2_Mass15
HLT_Photon42_R9Id85_OR_CaloId24b40e_Iso50T80L_Photon25_AND_HE10_R9Id65_Eta2_Mass15

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -14724,6 +14808,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30555/DoubleMuon_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30555/DoubleMuon_doc.html" + }, "date_created": [ "2016" ], @@ -14762,7 +14850,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-DoubleMuon-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu0
HLT_DoubleMu18NoFiltersNoVtx
HLT_DoubleMu23NoFiltersNoVtxDisplaced
HLT_DoubleMu28NoFiltersNoVtxDisplaced
HLT_DoubleMu33NoFiltersNoVtx
HLT_DoubleMu38NoFiltersNoVtx
HLT_DoubleMu8_Mass8_PFHT250
HLT_DoubleMu8_Mass8_PFHT300
HLT_L2DoubleMu23_NoVertex
HLT_L2DoubleMu28_NoVertex_2Cha_Angle2p5_Mass10
HLT_L2DoubleMu38_NoVertex_2Cha_Angle2p5_Mass10
HLT_Mu10_CentralPFJet30_BTagCSV_p13
HLT_Mu17_Mu8_DZ
HLT_Mu17_Mu8_SameSign_DZ
HLT_Mu17_Mu8_SameSign
HLT_Mu17_Mu8
HLT_Mu17_TkMu8_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL
HLT_Mu17
HLT_Mu20_Mu10_DZ
HLT_Mu20_Mu10_SameSign_DZ
HLT_Mu20_Mu10_SameSign
HLT_Mu20_Mu10
HLT_Mu27_TkMu8
HLT_Mu30_TkMu11
HLT_Mu3_PFJet40
HLT_Mu40_TkMu11
HLT_Mu8_TrkIsoVVL
HLT_Mu8
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_TripleMu_12_10_5
HLT_TripleMu_5_3_3_DZ_Mass3p8
HLT_TripleMu_5_3_3
HLT_TrkMu15_DoubleTrkMu5NoFiltersNoVtx
HLT_TrkMu17_DoubleTrkMu8NoFiltersNoVtx

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two energetic muons in the event.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-DoubleMuon-UL2016_MiniAODv2_NanoAODv9
Output dataset: /DoubleMuon/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DoubleMuon-UL2016_MiniAODv2
Output dataset: /DoubleMuon/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_DoubleMuon
Output dataset: /DoubleMuon/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu0
HLT_DoubleMu18NoFiltersNoVtx
HLT_DoubleMu23NoFiltersNoVtxDisplaced
HLT_DoubleMu28NoFiltersNoVtxDisplaced
HLT_DoubleMu33NoFiltersNoVtx
HLT_DoubleMu38NoFiltersNoVtx
HLT_DoubleMu8_Mass8_PFHT250
HLT_DoubleMu8_Mass8_PFHT300
HLT_L2DoubleMu23_NoVertex
HLT_L2DoubleMu28_NoVertex_2Cha_Angle2p5_Mass10
HLT_L2DoubleMu38_NoVertex_2Cha_Angle2p5_Mass10
HLT_Mu10_CentralPFJet30_BTagCSV_p13
HLT_Mu17_Mu8_DZ
HLT_Mu17_Mu8_SameSign_DZ
HLT_Mu17_Mu8_SameSign
HLT_Mu17_Mu8
HLT_Mu17_TkMu8_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_Mu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_Mu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_Mu17_TrkIsoVVL
HLT_Mu17
HLT_Mu20_Mu10_DZ
HLT_Mu20_Mu10_SameSign_DZ
HLT_Mu20_Mu10_SameSign
HLT_Mu20_Mu10
HLT_Mu27_TkMu8
HLT_Mu30_TkMu11
HLT_Mu3_PFJet40
HLT_Mu40_TkMu11
HLT_Mu8_TrkIsoVVL
HLT_Mu8
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL_DZ
HLT_TkMu17_TrkIsoVVL_TkMu8_TrkIsoVVL
HLT_TripleMu_12_10_5
HLT_TripleMu_5_3_3_DZ_Mass3p8
HLT_TripleMu_5_3_3
HLT_TrkMu15_DoubleTrkMu5NoFiltersNoVtx
HLT_TrkMu17_DoubleTrkMu8NoFiltersNoVtx

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -14961,6 +15049,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30556/DoubleMuonLowMass_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30556/DoubleMuonLowMass_doc.html" + }, "date_created": [ "2016" ], @@ -14999,7 +15091,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-DoubleMuonLowMass-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu3_Trk_Tau3mu
HLT_DoubleMu4_LowMassNonResonantTrk_Displaced

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons with low invariant mass.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-DoubleMuonLowMass-UL2016_MiniAODv2_NanoAODv9
Output dataset: /DoubleMuonLowMass/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-DoubleMuonLowMass-UL2016_MiniAODv2
Output dataset: /DoubleMuonLowMass/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step ReReco-Run2016H-DoubleMuonLowMass-21Feb2020_UL2016
Output dataset: /DoubleMuonLowMass/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMu3_Trk_Tau3mu
HLT_DoubleMu4_LowMassNonResonantTrk_Displaced

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -15198,6 +15290,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30557/HTMHT_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30557/HTMHT_doc.html" + }, "date_created": [ "2016" ], @@ -15236,7 +15332,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-HTMHT-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu140
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu80
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p57
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p63
HLT_PFHT200_PFAlphaT0p51
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p55
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p58
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p54
HLT_PFHT300_PFMET100
HLT_PFHT300_PFMET110
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p52
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p51
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p52
HLT_Rsq0p25
HLT_Rsq0p30
HLT_RsqMR240_Rsq0p09_MR200_4jet
HLT_RsqMR240_Rsq0p09_MR200
HLT_RsqMR270_Rsq0p09_MR200_4jet
HLT_RsqMR270_Rsq0p09_MR200

" + "description": "

Events stored in this primary dataset were selected because of the presence of a combination of a high scalar sum of the jet transverse momenta (HT), one or more energetic jets, or high missing transverse energy.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-HTMHT-UL2016_MiniAODv2_NanoAODv9
Output dataset: /HTMHT/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-HTMHT-UL2016_MiniAODv2
Output dataset: /HTMHT/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_HTMHT
Output dataset: /HTMHT/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu140
HLT_DiPFJet40_DEta3p5_MJJ600_PFMETNoMu80
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p57
HLT_PFHT200_DiPFJetAve90_PFAlphaT0p63
HLT_PFHT200_PFAlphaT0p51
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p55
HLT_PFHT250_DiPFJetAve90_PFAlphaT0p58
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT300_DiPFJetAve90_PFAlphaT0p54
HLT_PFHT300_PFMET100
HLT_PFHT300_PFMET110
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p52
HLT_PFHT350_DiPFJetAve90_PFAlphaT0p53
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p51
HLT_PFHT400_DiPFJetAve90_PFAlphaT0p52
HLT_Rsq0p25
HLT_Rsq0p30
HLT_RsqMR240_Rsq0p09_MR200_4jet
HLT_RsqMR240_Rsq0p09_MR200
HLT_RsqMR270_Rsq0p09_MR200_4jet
HLT_RsqMR270_Rsq0p09_MR200

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -15435,6 +15531,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30558/JetHT_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30558/JetHT_doc.html" + }, "date_created": [ "2016" ], @@ -15487,7 +15587,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-JetHT-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_AK8DiPFJet250_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet250_200_TrimMass30
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet280_200_TrimMass30
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet300_200_TrimMass30
HLT_AK8PFHT600_TrimR0p1PT0p03Mass50_BTagCSV_p20
HLT_AK8PFHT650_TrimR0p1PT0p03Mass50
HLT_AK8PFHT700_TrimR0p1PT0p03Mass50
HLT_AK8PFHT750_TrimMass50
HLT_AK8PFHT800_TrimMass50
HLT_AK8PFJet140
HLT_AK8PFJet200
HLT_AK8PFJet260
HLT_AK8PFJet320
HLT_AK8PFJet360_TrimMass30
HLT_AK8PFJet400_TrimMass30
HLT_AK8PFJet400
HLT_AK8PFJet40
HLT_AK8PFJet450
HLT_AK8PFJet500
HLT_AK8PFJet60
HLT_AK8PFJet80
HLT_CaloJet500_NoJetID
HLT_DiCentralPFJet170_CFMax0p1
HLT_DiCentralPFJet170
HLT_DiCentralPFJet220_CFMax0p3
HLT_DiCentralPFJet330_CFMax0p5
HLT_DiCentralPFJet430
HLT_DiJetVBFMu_PassThrough
HLT_DiJetVBF_PassThrough
HLT_DiPFJetAve100_HFJEC
HLT_DiPFJetAve140
HLT_DiPFJetAve160_HFJEC
HLT_DiPFJetAve200
HLT_DiPFJetAve220_HFJEC
HLT_DiPFJetAve260
HLT_DiPFJetAve300_HFJEC
HLT_DiPFJetAve320
HLT_DiPFJetAve400
HLT_DiPFJetAve40
HLT_DiPFJetAve500
HLT_DiPFJetAve60_HFJEC
HLT_DiPFJetAve60
HLT_DiPFJetAve80_HFJEC
HLT_DiPFJetAve80
HLT_HT2000
HLT_HT2500
HLT_L1_TripleJet_VBF
HLT_PFHT125
HLT_PFHT200
HLT_PFHT250
HLT_PFHT300
HLT_PFHT350
HLT_PFHT400_SixJet30_DoubleBTagCSV_p056
HLT_PFHT400_SixJet30
HLT_PFHT400
HLT_PFHT450_SixJet40_BTagCSV_p056
HLT_PFHT450_SixJet40
HLT_PFHT475
HLT_PFHT550_4JetPt50
HLT_PFHT600
HLT_PFHT650_4JetPt50
HLT_PFHT650_WideJetMJJ900DEtaJJ1p5
HLT_PFHT650_WideJetMJJ950DEtaJJ1p5
HLT_PFHT650
HLT_PFHT750_4JetPt50
HLT_PFHT750_4JetPt70
HLT_PFHT750_4JetPt80
HLT_PFHT800_4JetPt50
HLT_PFHT800
HLT_PFHT850_4JetPt50
HLT_PFHT900
HLT_PFJet140
HLT_PFJet200
HLT_PFJet260
HLT_PFJet320
HLT_PFJet400
HLT_PFJet40
HLT_PFJet450
HLT_PFJet500
HLT_PFJet60
HLT_PFJet80
HLT_QuadPFJet_VBF
HLT_SingleCentralPFJet170_CFMax0p1

" + "description": "

Events stored in this primary dataset were selected because of the presence of a high scalar sum of the jet transverse momenta (HT), or at least one or two energetic jets.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-JetHT-UL2016_MiniAODv2_NanoAODv9
Output dataset: /JetHT/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-JetHT-UL2016_MiniAODv2
Output dataset: /JetHT/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_JetHT
Output dataset: /JetHT/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_AK8DiPFJet250_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet250_200_TrimMass30
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet280_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet280_200_TrimMass30
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p087
HLT_AK8DiPFJet300_200_TrimMass30_BTagCSV_p20
HLT_AK8DiPFJet300_200_TrimMass30
HLT_AK8PFHT600_TrimR0p1PT0p03Mass50_BTagCSV_p20
HLT_AK8PFHT650_TrimR0p1PT0p03Mass50
HLT_AK8PFHT700_TrimR0p1PT0p03Mass50
HLT_AK8PFHT750_TrimMass50
HLT_AK8PFHT800_TrimMass50
HLT_AK8PFJet140
HLT_AK8PFJet200
HLT_AK8PFJet260
HLT_AK8PFJet320
HLT_AK8PFJet360_TrimMass30
HLT_AK8PFJet400_TrimMass30
HLT_AK8PFJet400
HLT_AK8PFJet40
HLT_AK8PFJet450
HLT_AK8PFJet500
HLT_AK8PFJet60
HLT_AK8PFJet80
HLT_CaloJet500_NoJetID
HLT_DiCentralPFJet170_CFMax0p1
HLT_DiCentralPFJet170
HLT_DiCentralPFJet220_CFMax0p3
HLT_DiCentralPFJet330_CFMax0p5
HLT_DiCentralPFJet430
HLT_DiJetVBFMu_PassThrough
HLT_DiJetVBF_PassThrough
HLT_DiPFJetAve100_HFJEC
HLT_DiPFJetAve140
HLT_DiPFJetAve160_HFJEC
HLT_DiPFJetAve200
HLT_DiPFJetAve220_HFJEC
HLT_DiPFJetAve260
HLT_DiPFJetAve300_HFJEC
HLT_DiPFJetAve320
HLT_DiPFJetAve400
HLT_DiPFJetAve40
HLT_DiPFJetAve500
HLT_DiPFJetAve60_HFJEC
HLT_DiPFJetAve60
HLT_DiPFJetAve80_HFJEC
HLT_DiPFJetAve80
HLT_HT2000
HLT_HT2500
HLT_L1_TripleJet_VBF
HLT_PFHT125
HLT_PFHT200
HLT_PFHT250
HLT_PFHT300
HLT_PFHT350
HLT_PFHT400_SixJet30_DoubleBTagCSV_p056
HLT_PFHT400_SixJet30
HLT_PFHT400
HLT_PFHT450_SixJet40_BTagCSV_p056
HLT_PFHT450_SixJet40
HLT_PFHT475
HLT_PFHT550_4JetPt50
HLT_PFHT600
HLT_PFHT650_4JetPt50
HLT_PFHT650_WideJetMJJ900DEtaJJ1p5
HLT_PFHT650_WideJetMJJ950DEtaJJ1p5
HLT_PFHT650
HLT_PFHT750_4JetPt50
HLT_PFHT750_4JetPt70
HLT_PFHT750_4JetPt80
HLT_PFHT800_4JetPt50
HLT_PFHT800
HLT_PFHT850_4JetPt50
HLT_PFHT900
HLT_PFJet140
HLT_PFJet200
HLT_PFJet260
HLT_PFJet320
HLT_PFJet400
HLT_PFJet40
HLT_PFJet450
HLT_PFJet500
HLT_PFJet60
HLT_PFJet80
HLT_QuadPFJet_VBF
HLT_SingleCentralPFJet170_CFMax0p1

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -15684,6 +15784,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30559/MET_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30559/MET_doc.html" + }, "date_created": [ "2016" ], @@ -15750,7 +15854,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-MET-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight_BTagCSV_p067
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight
HLT_DiCentralPFJet55_PFMET110
HLT_DoubleMu3_PFMET50
HLT_MET200
HLT_MET250
HLT_MET300
HLT_MET600
HLT_MET60_IsoTrk35_Loose
HLT_MET700
HLT_MET75_IsoTrk50
HLT_MET90_IsoTrk50
HLT_MonoCentralPFJet80_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_Mu14er_PFMET100
HLT_Mu3er_PFHT140_PFMET125
HLT_Mu6_PFHT200_PFMET100
HLT_Mu6_PFHT200_PFMET80_BTagCSV_p067
HLT_PFMET100_PFMHT100_IDTight_BeamHaloCleaned
HLT_PFMET100_PFMHT100_IDTight
HLT_PFMET110_PFMHT110_IDTight
HLT_PFMET120_BTagCSV_p067
HLT_PFMET120_Mu5
HLT_PFMET120_PFMHT120_IDTight
HLT_PFMET170_BeamHaloCleaned
HLT_PFMET170_HBHECleaned
HLT_PFMET170_HBHE_BeamHaloCleaned
HLT_PFMET170_JetIdCleaned
HLT_PFMET170_NoiseCleaned
HLT_PFMET170_NotCleaned
HLT_PFMET300
HLT_PFMET400
HLT_PFMET500
HLT_PFMET600
HLT_PFMET90_PFMHT90_IDTight
HLT_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_PFMETTypeOne190_HBHE_BeamHaloCleaned

" + "description": "

Events stored in this primary dataset were selected because of the presence of high missing transverse energy.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-MET-UL2016_MiniAODv2_NanoAODv9
Output dataset: /MET/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-MET-UL2016_MiniAODv2
Output dataset: /MET/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_MET
Output dataset: /MET/Run2016H-21Feb2020_UL2016-v2/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight_BTagCSV_p067
HLT_CaloMHTNoPU90_PFMET90_PFMHT90_IDTight
HLT_DiCentralPFJet55_PFMET110
HLT_DoubleMu3_PFMET50
HLT_MET200
HLT_MET250
HLT_MET300
HLT_MET600
HLT_MET60_IsoTrk35_Loose
HLT_MET700
HLT_MET75_IsoTrk50
HLT_MET90_IsoTrk50
HLT_MonoCentralPFJet80_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_MonoCentralPFJet80_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_Mu14er_PFMET100
HLT_Mu3er_PFHT140_PFMET125
HLT_Mu6_PFHT200_PFMET100
HLT_Mu6_PFHT200_PFMET80_BTagCSV_p067
HLT_PFMET100_PFMHT100_IDTight_BeamHaloCleaned
HLT_PFMET100_PFMHT100_IDTight
HLT_PFMET110_PFMHT110_IDTight
HLT_PFMET120_BTagCSV_p067
HLT_PFMET120_Mu5
HLT_PFMET120_PFMHT120_IDTight
HLT_PFMET170_BeamHaloCleaned
HLT_PFMET170_HBHECleaned
HLT_PFMET170_HBHE_BeamHaloCleaned
HLT_PFMET170_JetIdCleaned
HLT_PFMET170_NoiseCleaned
HLT_PFMET170_NotCleaned
HLT_PFMET300
HLT_PFMET400
HLT_PFMET500
HLT_PFMET600
HLT_PFMET90_PFMHT90_IDTight
HLT_PFMETNoMu100_PFMHTNoMu100_IDTight
HLT_PFMETNoMu110_PFMHTNoMu110_IDTight
HLT_PFMETNoMu120_PFMHTNoMu120_IDTight
HLT_PFMETNoMu90_PFMHTNoMu90_IDTight
HLT_PFMETTypeOne190_HBHE_BeamHaloCleaned

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -15949,6 +16053,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30560/MuOnia_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30560/MuOnia_doc.html" + }, "date_created": [ "2016" ], @@ -15987,7 +16095,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-MuOnia-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Phi_Barrel
HLT_Dimuon0_Upsilon_Muon
HLT_Dimuon13_Upsilon
HLT_Dimuon8_Upsilon_Barrel
HLT_Mu16_TkMu0_dEta18_Onia
HLT_Mu16_TkMu0_dEta18_Phi
HLT_Mu25_TkMu0_dEta18_Onia
HLT_Mu7p5_L2Mu2_Upsilon
HLT_Mu7p5_Track2_Upsilon
HLT_Mu7p5_Track3p5_Upsilon
HLT_Mu7p5_Track7_Upsilon
HLT_QuadMuon0_Dimuon0_Upsilon

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least two muons in the event requiring only very low energy and some requirements in the invariant mass for selecting low-mass resonances.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-MuOnia-UL2016_MiniAODv2_NanoAODv9
Output dataset: /MuOnia/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-MuOnia-UL2016_MiniAODv2
Output dataset: /MuOnia/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_MuOnia
Output dataset: /MuOnia/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Dimuon0_Phi_Barrel
HLT_Dimuon0_Upsilon_Muon
HLT_Dimuon13_Upsilon
HLT_Dimuon8_Upsilon_Barrel
HLT_Mu16_TkMu0_dEta18_Onia
HLT_Mu16_TkMu0_dEta18_Phi
HLT_Mu25_TkMu0_dEta18_Onia
HLT_Mu7p5_L2Mu2_Upsilon
HLT_Mu7p5_Track2_Upsilon
HLT_Mu7p5_Track3p5_Upsilon
HLT_Mu7p5_Track7_Upsilon
HLT_QuadMuon0_Dimuon0_Upsilon

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -16186,6 +16294,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30561/MuonEG_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30561/MuonEG_doc.html" + }, "date_created": [ "2016" ], @@ -16252,7 +16364,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-MuonEG-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiMu9_Ele9_CaloIdL_TrackIdL
HLT_Mu12_Photon25_CaloIdL_L1ISO
HLT_Mu12_Photon25_CaloIdL_L1OR
HLT_Mu12_Photon25_CaloIdL
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Mu17_Photon22_CaloIdL_L1ISO
HLT_Mu17_Photon30_CaloIdL_L1ISO
HLT_Mu17_Photon35_CaloIdL_L1ISO
HLT_Mu17_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23NoFiltersNoVtx_Photon23_CaloIdL
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL
HLT_Mu27_Ele37_CaloIdL_GsfTrkIdVL
HLT_Mu28NoFiltersNoVtxDisplaced_Photon28_CaloIdL
HLT_Mu30_Ele30_CaloIdL_GsfTrkIdVL
HLT_Mu33NoFiltersNoVtxDisplaced_Photon33_CaloIdL
HLT_Mu33_Ele33_CaloIdL_GsfTrkIdVL
HLT_Mu37_Ele27_CaloIdL_GsfTrkIdVL
HLT_Mu38NoFiltersNoVtx_Photon38_CaloIdL
HLT_Mu42NoFiltersNoVtx_Photon42_CaloIdL
HLT_Mu8_DiEle12_CaloIdL_TrackIdL
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_Mu8_TrkIsoVVL_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL

" + "description": "

Events stored in this primary dataset were selected because of the presence of one energetic muon and electron or photon.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-MuonEG-UL2016_MiniAODv2_NanoAODv9
Output dataset: /MuonEG/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-MuonEG-UL2016_MiniAODv2
Output dataset: /MuonEG/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_MuonEG
Output dataset: /MuonEG/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DiMu9_Ele9_CaloIdL_TrackIdL
HLT_Mu12_Photon25_CaloIdL_L1ISO
HLT_Mu12_Photon25_CaloIdL_L1OR
HLT_Mu12_Photon25_CaloIdL
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu12_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL
HLT_Mu17_Photon22_CaloIdL_L1ISO
HLT_Mu17_Photon30_CaloIdL_L1ISO
HLT_Mu17_Photon35_CaloIdL_L1ISO
HLT_Mu17_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23NoFiltersNoVtx_Photon23_CaloIdL
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele12_CaloIdL_TrackIdL_IsoVL
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu23_TrkIsoVVL_Ele8_CaloIdL_TrackIdL_IsoVL
HLT_Mu27_Ele37_CaloIdL_GsfTrkIdVL
HLT_Mu28NoFiltersNoVtxDisplaced_Photon28_CaloIdL
HLT_Mu30_Ele30_CaloIdL_GsfTrkIdVL
HLT_Mu33NoFiltersNoVtxDisplaced_Photon33_CaloIdL
HLT_Mu33_Ele33_CaloIdL_GsfTrkIdVL
HLT_Mu37_Ele27_CaloIdL_GsfTrkIdVL
HLT_Mu38NoFiltersNoVtx_Photon38_CaloIdL
HLT_Mu42NoFiltersNoVtx_Photon42_CaloIdL
HLT_Mu8_DiEle12_CaloIdL_TrackIdL
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT250
HLT_Mu8_Ele8_CaloIdM_TrackIdM_Mass8_PFHT300
HLT_Mu8_TrkIsoVVL_Ele17_CaloIdL_TrackIdL_IsoVL
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL_DZ
HLT_Mu8_TrkIsoVVL_Ele23_CaloIdL_TrackIdL_IsoVL

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -16451,6 +16563,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30562/SingleElectron_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30562/SingleElectron_doc.html" + }, "date_created": [ "2016" ], @@ -16531,7 +16647,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Ele105_CaloIdVT_GsfTrkIdT
HLT_Ele115_CaloIdVT_GsfTrkIdT
HLT_Ele145_CaloIdVT_GsfTrkIdT
HLT_Ele15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Ele15_IsoVVVL_PFHT350_PFMET50
HLT_Ele15_IsoVVVL_PFHT350
HLT_Ele15_IsoVVVL_PFHT400_PFMET50
HLT_Ele15_IsoVVVL_PFHT400
HLT_Ele15_IsoVVVL_PFHT600
HLT_Ele200_CaloIdVT_GsfTrkIdT
HLT_Ele20_eta2p1_WPLoose_Gsf_LooseIsoPFTau28
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau29
HLT_Ele22_eta2p1_WPLoose_Gsf
HLT_Ele23_WPLoose_Gsf_WHbbBoost
HLT_Ele23_WPLoose_Gsf
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau30
HLT_Ele24_eta2p1_WPLoose_Gsf
HLT_Ele250_CaloIdVT_GsfTrkIdT
HLT_Ele25_WPTight_Gsf
HLT_Ele25_eta2p1_WPLoose_Gsf
HLT_Ele25_eta2p1_WPTight_Gsf
HLT_Ele27_WPLoose_Gsf_WHbbBoost
HLT_Ele27_WPLoose_Gsf
HLT_Ele27_WPTight_Gsf_L1JetTauSeeded
HLT_Ele27_WPTight_Gsf
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_HT200
HLT_Ele27_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele27_eta2p1_WPLoose_Gsf
HLT_Ele27_eta2p1_WPTight_Gsf
HLT_Ele300_CaloIdVT_GsfTrkIdT
HLT_Ele30_WPTight_Gsf
HLT_Ele30_eta2p1_WPTight_Gsf
HLT_Ele32_WPTight_Gsf
HLT_Ele32_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele32_eta2p1_WPTight_Gsf
HLT_Ele35_CaloIdVT_GsfTrkIdT_PFJet150_PFJet50
HLT_Ele35_WPLoose_Gsf
HLT_Ele36_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele45_CaloIdVT_GsfTrkIdT_PFJet200_PFJet50
HLT_Ele45_WPLoose_Gsf_L1JetTauSeeded
HLT_Ele45_WPLoose_Gsf
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet140
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet165
HLT_Ele50_IsoVVVL_PFHT400

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one high-energy electron, or at least one high-energy electron and one or more jets or tau.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2_NanoAODv9
Output dataset: /SingleElectron/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2
Output dataset: /SingleElectron/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_SingleElectron
Output dataset: /SingleElectron/Run2016H-21Feb2020_UL2016-v2/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Ele105_CaloIdVT_GsfTrkIdT
HLT_Ele115_CaloIdVT_GsfTrkIdT
HLT_Ele145_CaloIdVT_GsfTrkIdT
HLT_Ele15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Ele15_IsoVVVL_PFHT350_PFMET50
HLT_Ele15_IsoVVVL_PFHT350
HLT_Ele15_IsoVVVL_PFHT400_PFMET50
HLT_Ele15_IsoVVVL_PFHT400
HLT_Ele15_IsoVVVL_PFHT600
HLT_Ele200_CaloIdVT_GsfTrkIdT
HLT_Ele20_eta2p1_WPLoose_Gsf_LooseIsoPFTau28
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele22_eta2p1_WPLoose_Gsf_LooseIsoPFTau29
HLT_Ele22_eta2p1_WPLoose_Gsf
HLT_Ele23_WPLoose_Gsf_WHbbBoost
HLT_Ele23_WPLoose_Gsf
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau20
HLT_Ele24_eta2p1_WPLoose_Gsf_LooseIsoPFTau30
HLT_Ele24_eta2p1_WPLoose_Gsf
HLT_Ele250_CaloIdVT_GsfTrkIdT
HLT_Ele25_WPTight_Gsf
HLT_Ele25_eta2p1_WPLoose_Gsf
HLT_Ele25_eta2p1_WPTight_Gsf
HLT_Ele27_WPLoose_Gsf_WHbbBoost
HLT_Ele27_WPLoose_Gsf
HLT_Ele27_WPTight_Gsf_L1JetTauSeeded
HLT_Ele27_WPTight_Gsf
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_Ele27_eta2p1_WPLoose_Gsf_HT200
HLT_Ele27_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele27_eta2p1_WPLoose_Gsf
HLT_Ele27_eta2p1_WPTight_Gsf
HLT_Ele300_CaloIdVT_GsfTrkIdT
HLT_Ele30_WPTight_Gsf
HLT_Ele30_eta2p1_WPTight_Gsf
HLT_Ele32_WPTight_Gsf
HLT_Ele32_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele32_eta2p1_WPTight_Gsf
HLT_Ele35_CaloIdVT_GsfTrkIdT_PFJet150_PFJet50
HLT_Ele35_WPLoose_Gsf
HLT_Ele36_eta2p1_WPLoose_Gsf_LooseIsoPFTau20_SingleL1
HLT_Ele45_CaloIdVT_GsfTrkIdT_PFJet200_PFJet50
HLT_Ele45_WPLoose_Gsf_L1JetTauSeeded
HLT_Ele45_WPLoose_Gsf
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet140
HLT_Ele50_CaloIdVT_GsfTrkIdT_PFJet165
HLT_Ele50_IsoVVVL_PFHT400

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -16731,6 +16847,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30563/SingleMuon_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30563/SingleMuon_doc.html" + }, "date_created": [ "2016" ], @@ -16825,7 +16945,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-SingleMuon-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleIsoMu17_eta2p1_noDzCut
HLT_DoubleIsoMu17_eta2p1
HLT_IsoMu16_eta2p1_MET30_LooseIsoPFTau50_Trk30_eta2p1
HLT_IsoMu16_eta2p1_MET30
HLT_IsoMu17_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu17_eta2p1_LooseIsoPFTau20
HLT_IsoMu18
HLT_IsoMu19_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu19_eta2p1_LooseIsoPFTau20
HLT_IsoMu19_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu20
HLT_IsoMu21_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu21_eta2p1_LooseIsoPFTau50_Trk30_eta2p1_SingleL1
HLT_IsoMu21_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu22_eta2p1
HLT_IsoMu22
HLT_IsoMu24_eta2p1
HLT_IsoMu24
HLT_IsoMu27
HLT_IsoTkMu18
HLT_IsoTkMu20
HLT_IsoTkMu22_eta2p1
HLT_IsoTkMu22
HLT_IsoTkMu24_eta2p1
HLT_IsoTkMu24
HLT_IsoTkMu27
HLT_L1SingleMu16
HLT_L1SingleMu18
HLT_L2Mu10
HLT_Mu10_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT350_PFMETNoMu60
HLT_Mu15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Mu15_IsoVVVL_PFHT350_PFMET50
HLT_Mu15_IsoVVVL_PFHT350
HLT_Mu15_IsoVVVL_PFHT400_PFMET50
HLT_Mu15_IsoVVVL_PFHT400
HLT_Mu15_IsoVVVL_PFHT600
HLT_Mu16_eta2p1_MET30
HLT_Mu20
HLT_Mu24_eta2p1
HLT_Mu27
HLT_Mu28NoFiltersNoVtx_CentralCaloJet40
HLT_Mu28NoFiltersNoVtx_DisplacedJet40_Loose
HLT_Mu300
HLT_Mu30_eta2p1_PFJet150_PFJet50
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Loose
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Tight
HLT_Mu350
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Loose
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Tight
HLT_Mu38NoFiltersNoVtx_DisplacedJet60_Loose
HLT_Mu40_eta2p1_PFJet200_PFJet50
HLT_Mu45_eta2p1
HLT_Mu50_IsoVVVL_PFHT400
HLT_Mu50
HLT_Mu55
HLT_Mu8_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT300_PFMETNoMu60
HLT_TkMu17
HLT_TkMu20
HLT_TkMu24_eta2p1
HLT_TkMu27
HLT_TkMu50

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one energetic muon, or at least one muon and one or more jets, tau or high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-SingleMuon-UL2016_MiniAODv2_NanoAODv9
Output dataset: /SingleMuon/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-SingleMuon-UL2016_MiniAODv2
Output dataset: /SingleMuon/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_SingleMuon
Output dataset: /SingleMuon/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleIsoMu17_eta2p1_noDzCut
HLT_DoubleIsoMu17_eta2p1
HLT_IsoMu16_eta2p1_MET30_LooseIsoPFTau50_Trk30_eta2p1
HLT_IsoMu16_eta2p1_MET30
HLT_IsoMu17_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu17_eta2p1_LooseIsoPFTau20
HLT_IsoMu18
HLT_IsoMu19_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu19_eta2p1_LooseIsoPFTau20
HLT_IsoMu19_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu20
HLT_IsoMu21_eta2p1_LooseIsoPFTau20_SingleL1
HLT_IsoMu21_eta2p1_LooseIsoPFTau50_Trk30_eta2p1_SingleL1
HLT_IsoMu21_eta2p1_MediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu22_eta2p1
HLT_IsoMu22
HLT_IsoMu24_eta2p1
HLT_IsoMu24
HLT_IsoMu27
HLT_IsoTkMu18
HLT_IsoTkMu20
HLT_IsoTkMu22_eta2p1
HLT_IsoTkMu22
HLT_IsoTkMu24_eta2p1
HLT_IsoTkMu24
HLT_IsoTkMu27
HLT_L1SingleMu16
HLT_L1SingleMu18
HLT_L2Mu10
HLT_Mu10_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT350_PFMETNoMu60
HLT_Mu15_IsoVVVL_BTagCSV_p067_PFHT400
HLT_Mu15_IsoVVVL_PFHT350_PFMET50
HLT_Mu15_IsoVVVL_PFHT350
HLT_Mu15_IsoVVVL_PFHT400_PFMET50
HLT_Mu15_IsoVVVL_PFHT400
HLT_Mu15_IsoVVVL_PFHT600
HLT_Mu16_eta2p1_MET30
HLT_Mu20
HLT_Mu24_eta2p1
HLT_Mu27
HLT_Mu28NoFiltersNoVtx_CentralCaloJet40
HLT_Mu28NoFiltersNoVtx_DisplacedJet40_Loose
HLT_Mu300
HLT_Mu30_eta2p1_PFJet150_PFJet50
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Loose
HLT_Mu33NoFiltersNoVtxDisplaced_DisplacedJet50_Tight
HLT_Mu350
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Loose
HLT_Mu38NoFiltersNoVtxDisplaced_DisplacedJet60_Tight
HLT_Mu38NoFiltersNoVtx_DisplacedJet60_Loose
HLT_Mu40_eta2p1_PFJet200_PFJet50
HLT_Mu45_eta2p1
HLT_Mu50_IsoVVVL_PFHT400
HLT_Mu50
HLT_Mu55
HLT_Mu8_TrkIsoVVL_DiPFJet40_DEta3p5_MJJ750_HTT300_PFMETNoMu60
HLT_TkMu17
HLT_TkMu20
HLT_TkMu24_eta2p1
HLT_TkMu27
HLT_TkMu50

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -17024,6 +17144,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30564/SinglePhoton_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30564/SinglePhoton_doc.html" + }, "date_created": [ "2016" ], @@ -17062,7 +17186,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-SinglePhoton-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon120_R9Id90_HE10_IsoM
HLT_Photon120
HLT_Photon135_PFMET100
HLT_Photon165_HE10
HLT_Photon165_R9Id90_HE10_IsoM
HLT_Photon175
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon22_R9Id90_HE10_IsoM
HLT_Photon22
HLT_Photon250_NoHE
HLT_Photon300_NoHE
HLT_Photon30_R9Id90_HE10_IsoM
HLT_Photon30
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon36_R9Id90_HE10_IsoM
HLT_Photon36
HLT_Photon500
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon50_R9Id90_HE10_IsoM
HLT_Photon50
HLT_Photon600
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon75_R9Id90_HE10_IsoM
HLT_Photon75
HLT_Photon90_CaloIdL_PFHT500
HLT_Photon90_CaloIdL_PFHT600
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon90_R9Id90_HE10_IsoM
HLT_Photon90

" + "description": "

Events stored in this primary dataset were selected because of the presence of one energetic photon, or one photon and high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-SinglePhoton-UL2016_MiniAODv2_NanoAODv9
Output dataset: /SinglePhoton/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-SinglePhoton-UL2016_MiniAODv2
Output dataset: /SinglePhoton/Run2016H-UL2016_MiniAODv2-v2/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_SinglePhoton
Output dataset: /SinglePhoton/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon120_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon120_R9Id90_HE10_IsoM
HLT_Photon120
HLT_Photon135_PFMET100
HLT_Photon165_HE10
HLT_Photon165_R9Id90_HE10_IsoM
HLT_Photon175
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon22_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon22_R9Id90_HE10_IsoM
HLT_Photon22
HLT_Photon250_NoHE
HLT_Photon300_NoHE
HLT_Photon30_R9Id90_HE10_IsoM
HLT_Photon30
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon36_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon36_R9Id90_HE10_IsoM
HLT_Photon36
HLT_Photon500
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon50_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon50_R9Id90_HE10_IsoM
HLT_Photon50
HLT_Photon600
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon75_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon75_R9Id90_HE10_IsoM
HLT_Photon75
HLT_Photon90_CaloIdL_PFHT500
HLT_Photon90_CaloIdL_PFHT600
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_PFMET40
HLT_Photon90_R9Id90_HE10_Iso40_EBOnly_VBF
HLT_Photon90_R9Id90_HE10_IsoM
HLT_Photon90

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", @@ -17262,6 +17386,10 @@ "energy": "13TeV", "type": "pp" }, + "dataset_semantics_files": { + "json": "/eos/opendata/cms/dataset-semantics/NanoAOD/30565/Tau_doc.json", + "url": "/eos/opendata/cms/dataset-semantics/NanoAOD/30565/Tau_doc.html" + }, "date_created": [ "2016" ], @@ -17300,7 +17428,7 @@ "attribution": "CC0" }, "methodology": { - "description": "

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing / NANO
This primary NANOAOD dataset was processed from the MINIAOD dataset by the following step:
Step: NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-Tau-UL2016_MiniAODv2_NanoAODv9\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMediumCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1
HLT_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1
HLT_IsoMu19_eta2p1_LooseCombinedIsoPFTau20
HLT_IsoMu19_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu19_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET110
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET120
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET80
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET90
HLT_LooseIsoPFTau50_Trk30_eta2p1
HLT_PFTau120_eta2p1
HLT_PFTau140_eta2p1
HLT_VLooseIsoPFTau120_Trk50_eta2p1
HLT_VLooseIsoPFTau140_Trk50_eta2p1

" + "description": "

Events stored in this primary dataset were selected because of the presence of at least one tau, or one tau and muon or high missing transverse momentum.

Data taking / HLT
The collision data were assigned to different RAW datasets using the following HLT configuration.

Data processing
This NANOAOD dataset was processed from the RAW dataset by the following steps:

Step NANO
Release: CMSSW_10_6_26
Global tag: 106X_dataRun2_v35\n
Configuration file for NANO step ReReco-Run2016H-Tau-UL2016_MiniAODv2_NanoAODv9
Output dataset: /Tau/Run2016H-UL2016_MiniAODv2_NanoAODv9-v1/NANOAOD\n


Step PAT
Release: CMSSW_10_6_25
Global tag: 106X_dataRun2_v35\n
Configuration file for PAT step ReReco-Run2016H-Tau-UL2016_MiniAODv2
Output dataset: /Tau/Run2016H-UL2016_MiniAODv2-v1/MINIAOD\n


Step RECO
Release: CMSSW_10_6_8_patch1
Global tag: 106X_dataRun2_v27\n
Configuration file for RECO step recoskim_Run2016H_Tau
Output dataset: /Tau/Run2016H-21Feb2020_UL2016-v1/AOD\n

HLT trigger paths
The possible HLT trigger paths in this dataset are:
HLT_DoubleMediumCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleMediumCombinedIsoPFTau40_Trk1_eta2p1
HLT_DoubleMediumIsoPFTau32_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleMediumIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau35_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1_Reg
HLT_DoubleTightCombinedIsoPFTau40_Trk1_eta2p1
HLT_IsoMu19_eta2p1_LooseCombinedIsoPFTau20
HLT_IsoMu19_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu19_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_MediumCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_IsoMu21_eta2p1_TightCombinedIsoPFTau32_Trk1_eta2p1_Reg
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET110
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET120
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET80
HLT_LooseIsoPFTau50_Trk30_eta2p1_MET90
HLT_LooseIsoPFTau50_Trk30_eta2p1
HLT_PFTau120_eta2p1
HLT_PFTau140_eta2p1
HLT_VLooseIsoPFTau120_Trk50_eta2p1
HLT_VLooseIsoPFTau140_Trk50_eta2p1

" }, "note": { "description": "The list of validated runs, which must be applied to all analyses, can be found in", diff --git a/cernopendata/modules/fixtures/data/records/cms-reco-configuration-files-2015.json b/cernopendata/modules/fixtures/data/records/cms-reco-configuration-files-2015.json index 090c26bcaf..b12a6a1e0c 100644 --- a/cernopendata/modules/fixtures/data/records/cms-reco-configuration-files-2015.json +++ b/cernopendata/modules/fixtures/data/records/cms-reco-configuration-files-2015.json @@ -30,7 +30,7 @@ ], "files": [ { - "checksum": "adler32:a48dd1062517325932854f3bad3cffd376618dd8", + "checksum": "adler32:5268c3c8", "size": 10000, "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2015/reco_2015D_Charmonium.py" } @@ -82,7 +82,7 @@ ], "files": [ { - "checksum": "adler32:ae7defe3a6fab273ebd489b8f82342fe35872fa7", + "checksum": "adler32:bc393891", "size": 15946, "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2015/reco_2015D_SingleMuon.py" } @@ -134,7 +134,7 @@ ], "files": [ { - 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It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." + }, + "publisher": "CERN Open Data Portal", + "recid": "30443", + "run_period": [ + "Run2016G" + ], + "title": "Configuration file for PAT step ReReco-Run2016G-BTagCSV-UL2016_MiniAODv2", + "type": { + "primary": "Supplementaries", + "secondary": [ + "Configuration" + ] + } + }, + { + "abstract": { + "description": "The configuration file used in PAT data processing step." + }, + "accelerator": "CERN-LHC", + "collaboration": { + "name": "CMS Collaboration", + "recid": "" + }, + "collections": [ + "CMS-Configuration-Files" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "py" + ], + "number_files": 1, + "size": 10038 + }, + "experiment": [ + "CMS" + ], + "files": [ + { + "checksum": "adler32:f4969d43", + "size": 10038, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-DoubleMuonLowMass-UL2016_MiniAODv2.py" + } + ], + "note": { + "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." + }, + "publisher": "CERN Open Data Portal", + "recid": "30444", + "run_period": [ + "Run2016H" + ], + "title": "Configuration file for PAT step ReReco-Run2016H-DoubleMuonLowMass-UL2016_MiniAODv2", + "type": { + "primary": "Supplementaries", + "secondary": [ + "Configuration" + ] + } + }, + { + "abstract": { + "description": "The configuration file used in PAT data processing step." + }, + "accelerator": "CERN-LHC", + "collaboration": { + "name": "CMS Collaboration", + "recid": "" + }, + "collections": [ + "CMS-Configuration-Files" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "py" + ], + "number_files": 1, + "size": 10023 + }, + "experiment": [ + "CMS" + ], + "files": [ + { + "checksum": "adler32:c9bb978e", + "size": 10023, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-SinglePhoton-UL2016_MiniAODv2.py" + } + ], + "note": { + "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. 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It is provided only for information purposes. 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Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30446", + "recid": "30496", "run_period": [ - "Run2016G" + "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016G-MuonEG-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016H_DoubleMuon", "type": { "primary": "Supplementaries", "secondary": [ @@ -2492,7 +5142,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -2503,7 +5153,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -2515,27 +5165,27 @@ "py" ], "number_files": 1, - "size": 4257 + "size": 73534 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:e8d347336a755534ba8878226a94b0453ec7822d", - "size": 4257, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-SinglePhoton-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:db48ba19", + "size": 73534, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_JetHT.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. 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Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30447", + "recid": "30497", "run_period": [ "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016H-SinglePhoton-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016H_JetHT", "type": { "primary": "Supplementaries", "secondary": [ @@ -2545,7 +5195,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -2556,7 +5206,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -2568,27 +5218,27 @@ "py" ], "number_files": 1, - "size": 4251 + "size": 93063 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:ca7cb920d3fffa5699132d3fe32726365f581381", - "size": 4251, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-SingleMuon-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:9a98f04f", + "size": 93063, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_MET.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30448", + "recid": "30498", "run_period": [ - "Run2016G" + "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016G-SingleMuon-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016H_MET", "type": { "primary": "Supplementaries", "secondary": [ @@ -2598,7 +5248,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -2609,7 +5259,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -2621,27 +5271,27 @@ "py" ], "number_files": 1, - "size": 4230 + "size": 55032 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:ddedffe8bfe8871c93a87b9c0a10dc6eabf4ff05", - "size": 4230, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-MET-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:2c496521", + "size": 55032, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_SingleElectron.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30449", + "recid": "30499", "run_period": [ "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016H-MET-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016H_SingleElectron", "type": { "primary": "Supplementaries", "secondary": [ @@ -2651,7 +5301,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -2662,7 +5312,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -2674,27 +5324,27 @@ "py" ], "number_files": 1, - "size": 4239 + "size": 89997 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:3f784d199ef4fb1a305cae09456d0f17f79c3550", - "size": 4239, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-MuonEG-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:3d04f21f", + "size": 89997, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_SingleMuon.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30450", + "recid": "30566", "run_period": [ "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016H-MuonEG-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016H_SingleMuon", "type": { "primary": "Supplementaries", "secondary": [ @@ -2704,7 +5354,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -2715,7 +5365,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -2727,27 +5377,27 @@ "py" ], "number_files": 1, - "size": 4263 + "size": 47428 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:1b50054093f5fc1a0197c0e6ed3fe808438cad4f", - "size": 4263, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:b8de99af", + "size": 47428, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_ZeroBias.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30451", + "recid": "30567", "run_period": [ "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016H_ZeroBias", "type": { "primary": "Supplementaries", "secondary": [ @@ -2768,7 +5418,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -2780,27 +5430,27 @@ "py" ], "number_files": 1, - "size": 4251 + "size": 4230 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:a8cca218492bc676cb326a5906118a37dc673277", - "size": 4251, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-SingleMuon-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:fda6d0bc", + "size": 4230, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-MET-UL2016_MiniAODv2_NanoAODv9.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30452", + "recid": "30568", "run_period": [ - "Run2016H" + "Run2016G" ], - "title": "Configuration file for NANO step ReReco-Run2016H-SingleMuon-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for NANO step ReReco-Run2016G-MET-UL2016_MiniAODv2_NanoAODv9", "type": { "primary": "Supplementaries", "secondary": [ @@ -2821,7 +5471,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -2833,27 +5483,27 @@ "py" ], "number_files": 1, - "size": 4230 + "size": 4239 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:24c1d71ad326f15032d4e6c82d7981c573c8a7e6", - "size": 4230, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-Tau-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:6ff0d4eb", + "size": 4239, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-MuOnia-UL2016_MiniAODv2_NanoAODv9.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30453", + "recid": "30569", "run_period": [ "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016H-Tau-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for NANO step ReReco-Run2016H-MuOnia-UL2016_MiniAODv2_NanoAODv9", "type": { "primary": "Supplementaries", "secondary": [ @@ -2874,7 +5524,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -2886,27 +5536,27 @@ "py" ], "number_files": 1, - "size": 4245 + "size": 4251 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:4cba9c2d1a12656a95bd4ab5dc9fb8a4cd2f5dd0", - "size": 4245, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-DoubleEG-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:69b1d9fe", + "size": 4251, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-DoubleMuon-UL2016_MiniAODv2_NanoAODv9.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30454", + "recid": "30570", "run_period": [ "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016H-DoubleEG-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for NANO step ReReco-Run2016H-DoubleMuon-UL2016_MiniAODv2_NanoAODv9", "type": { "primary": "Supplementaries", "secondary": [ @@ -2927,7 +5577,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -2939,27 +5589,27 @@ "py" ], "number_files": 1, - "size": 10029 + "size": 10017 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:169321b92dffe2ab3c03a1e0fbb693fa96c0fb9f", - "size": 10029, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-SingleElectron-UL2016_MiniAODv2.py" + "checksum": "adler32:4b079536", + "size": 10017, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-Charmonium-UL2016_MiniAODv2.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30455", + "recid": "30571", "run_period": [ "Run2016G" ], - "title": "Configuration file for PAT step ReReco-Run2016G-SingleElectron-UL2016_MiniAODv2", + "title": "Configuration file for PAT step ReReco-Run2016G-Charmonium-UL2016_MiniAODv2", "type": { "primary": "Supplementaries", "secondary": [ @@ -2969,7 +5619,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in PAT data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -2980,7 +5630,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -2992,27 +5642,27 @@ "py" ], "number_files": 1, - "size": 4272 + "size": 9912 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:7c6d62488a08a45fe614c0aa98d6bcf7f1b06860", - "size": 4272, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-DoubleMuonLowMass-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:151671c0", + "size": 9912, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-DisplacedJet-UL2016_MiniAODv2.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30456", + "recid": "30572", "run_period": [ "Run2016G" ], - "title": "Configuration file for NANO step ReReco-Run2016G-DoubleMuonLowMass-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for PAT step ReReco-Run2016G-DisplacedJet-UL2016_MiniAODv2", "type": { "primary": "Supplementaries", "secondary": [ @@ -3033,7 +5683,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3045,27 +5695,27 @@ "py" ], "number_files": 1, - "size": 10011 + "size": 9912 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:7244d3924ff55dd0ac65e2d2566377c272368a47", - "size": 10011, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-ZeroBias-UL2016_MiniAODv2.py" + "checksum": "adler32:7c9a71c3", + "size": 9912, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-DisplacedJet-UL2016_MiniAODv2.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30457", + "recid": "30573", "run_period": [ "Run2016H" ], - "title": "Configuration file for PAT step ReReco-Run2016H-ZeroBias-UL2016_MiniAODv2", + "title": "Configuration file for PAT step ReReco-Run2016H-DisplacedJet-UL2016_MiniAODv2", "type": { "primary": "Supplementaries", "secondary": [ @@ -3086,7 +5736,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3098,27 +5748,27 @@ "py" ], "number_files": 1, - "size": 10011 + "size": 9894 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:4dfad2d5b1f57b899d2277c4f7516efc8be287f8", - "size": 10011, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-ZeroBias-UL2016_MiniAODv2.py" + "checksum": "adler32:2bac6a97", + "size": 9894, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-MuOnia-UL2016_MiniAODv2.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30458", + "recid": "30574", "run_period": [ "Run2016G" ], - "title": "Configuration file for PAT step ReReco-Run2016G-ZeroBias-UL2016_MiniAODv2", + "title": "Configuration file for PAT step ReReco-Run2016G-MuOnia-UL2016_MiniAODv2", "type": { "primary": "Supplementaries", "secondary": [ @@ -3128,7 +5778,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3139,7 +5789,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3151,27 +5801,27 @@ "py" ], "number_files": 1, - "size": 4672 + "size": 41858 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:fbba5ead035451e9ad8cf7c7eef01b5d3d2c8b4a", - "size": 4672, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-ZeroBias-UL2016_MiniAODv2_JMENanoAODv9.py" + "checksum": "adler32:9456801d", + "size": 41858, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016G_BTagCSV.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30459", + "recid": "30575", "run_period": [ "Run2016G" ], - "title": "Configuration file for NANO step ReReco-Run2016G-ZeroBias-UL2016_MiniAODv2_JMENanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016G_BTagCSV", "type": { "primary": "Supplementaries", "secondary": [ @@ -3181,7 +5831,7 @@ }, { "abstract": { - "description": "The configuration file used in PAT data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3192,7 +5842,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3204,27 +5854,27 @@ "py" ], "number_files": 1, - "size": 10038 + "size": 41857 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:895e37339ffbcfeca1de8e6e1d6f34744537a250", - "size": 10038, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-DoubleMuonLowMass-UL2016_MiniAODv2.py" + "checksum": "adler32:516b7ff3", + "size": 41857, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016G_BTagMu.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30460", + "recid": "30576", "run_period": [ "Run2016G" ], - "title": "Configuration file for PAT step ReReco-Run2016G-DoubleMuonLowMass-UL2016_MiniAODv2", + "title": "Configuration file for RECO step recoskim_Run2016G_BTagMu", "type": { "primary": "Supplementaries", "secondary": [ @@ -3234,7 +5884,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3245,7 +5895,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3257,27 +5907,27 @@ "py" ], "number_files": 1, - "size": 4251 + "size": 45336 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:13eadf3812ff47499eac28848d9e6654339de5df", - "size": 4251, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-Charmonium-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:f986ca80", + "size": 45336, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016G_Charmonium.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30461", + "recid": "30577", "run_period": [ - "Run2016H" + "Run2016G" ], - "title": "Configuration file for NANO step ReReco-Run2016H-Charmonium-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016G_Charmonium", "type": { "primary": "Supplementaries", "secondary": [ @@ -3287,7 +5937,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3298,7 +5948,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3310,27 +5960,27 @@ "py" ], "number_files": 1, - "size": 4251 + "size": 41863 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:fa2df9f335fa2327446081d993af58794dba422f", - "size": 4251, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-DoubleMuon-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:abaf827f", + "size": 41863, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016G_DisplacedJet.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30462", + "recid": "30578", "run_period": [ "Run2016G" ], - "title": "Configuration file for NANO step ReReco-Run2016G-DoubleMuon-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016G_DisplacedJet", "type": { "primary": "Supplementaries", "secondary": [ @@ -3340,7 +5990,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3351,7 +6001,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3363,27 +6013,27 @@ "py" ], "number_files": 1, - "size": 4236 + "size": 41856 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:f29c00bb05da4382f76a568231586aab068d0378", - "size": 4236, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-JetHT-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:f0137f58", + "size": 41856, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016G_HTMHT.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30463", + "recid": "30579", "run_period": [ "Run2016G" ], - "title": "Configuration file for NANO step ReReco-Run2016G-JetHT-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016G_HTMHT", "type": { "primary": "Supplementaries", "secondary": [ @@ -3393,7 +6043,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3404,7 +6054,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3416,27 +6066,27 @@ "py" ], "number_files": 1, - "size": 4263 + "size": 44203 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:6ce9228ff38a4f36f43ad47f596a5692b0aa5358", - "size": 4263, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-SingleElectron-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:aeb36c93", + "size": 44203, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016G_MuOnia.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30464", + "recid": "30580", "run_period": [ "Run2016G" ], - "title": "Configuration file for NANO step ReReco-Run2016G-SingleElectron-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016G_MuOnia", "type": { "primary": "Supplementaries", "secondary": [ @@ -3446,7 +6096,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3457,7 +6107,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3469,27 +6119,27 @@ "py" ], "number_files": 1, - "size": 4242 + "size": 69594 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:7b29747770d5add9e730d8dda2839b65bdf83137", - "size": 4242, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-BTagCSV-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:7ea4b67b", + "size": 69594, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016G_MuonEG.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30465", + "recid": "30581", "run_period": [ "Run2016G" ], - "title": "Configuration file for NANO step ReReco-Run2016G-BTagCSV-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016G_MuonEG", "type": { "primary": "Supplementaries", "secondary": [ @@ -3499,7 +6149,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3510,7 +6160,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3522,27 +6172,27 @@ "py" ], "number_files": 1, - "size": 4672 + "size": 95212 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:b34d99ace9eed68bed043700aa7bd8817443eaa9", - "size": 4672, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-ZeroBias-UL2016_MiniAODv2_JMENanoAODv9.py" + "checksum": "adler32:a7a3cf9e", + "size": 95212, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016G_SinglePhoton.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30466", + "recid": "30582", "run_period": [ - "Run2016H" + "Run2016G" ], - "title": "Configuration file for NANO step ReReco-Run2016H-ZeroBias-UL2016_MiniAODv2_JMENanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016G_SinglePhoton", "type": { "primary": "Supplementaries", "secondary": [ @@ -3552,7 +6202,7 @@ }, { "abstract": { - "description": "The configuration file used in PAT data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3563,7 +6213,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3575,27 +6225,27 @@ "py" ], "number_files": 1, - "size": 10029 + "size": 41854 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:418c1582e3b5aa9383f97838df65324eb5c73cee", - "size": 10029, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2.py" + "checksum": "adler32:44d7efd", + "size": 41854, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016G_Tau.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30467", + "recid": "30583", "run_period": [ - "Run2016H" + "Run2016G" ], - "title": "Configuration file for PAT step ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2", + "title": "Configuration file for RECO step recoskim_Run2016G_Tau", "type": { "primary": "Supplementaries", "secondary": [ @@ -3605,7 +6255,7 @@ }, { "abstract": { - "description": "The configuration file used in PAT data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3616,7 +6266,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3628,27 +6278,27 @@ "py" ], "number_files": 1, - "size": 10017 + "size": 41858 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:09d35c4bd082e69036fb567c08e71244edb2d607", - "size": 10017, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-SingleMuon-UL2016_MiniAODv2.py" + "checksum": "adler32:3582801e", + "size": 41858, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_BTagCSV.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30468", + "recid": "30584", "run_period": [ - "Run2016G" + "Run2016H" ], - "title": "Configuration file for PAT step ReReco-Run2016G-SingleMuon-UL2016_MiniAODv2", + "title": "Configuration file for RECO step recoskim_Run2016H_BTagCSV", "type": { "primary": "Supplementaries", "secondary": [ @@ -3658,7 +6308,7 @@ }, { "abstract": { - "description": "The configuration file used in PAT data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3669,7 +6319,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3681,27 +6331,27 @@ "py" ], "number_files": 1, - "size": 10017 + "size": 41857 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:8ef48b84eb6d8d5580e083f0cc2738a33a85f5b9", - "size": 10017, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-SingleMuon-UL2016_MiniAODv2.py" + "checksum": "adler32:f2877ff4", + "size": 41857, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_BTagMu.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30469", + "recid": "30585", "run_period": [ "Run2016H" ], - "title": "Configuration file for PAT step ReReco-Run2016H-SingleMuon-UL2016_MiniAODv2", + "title": "Configuration file for RECO step recoskim_Run2016H_BTagMu", "type": { "primary": "Supplementaries", "secondary": [ @@ -3711,7 +6361,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3722,7 +6372,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3734,27 +6384,27 @@ "py" ], "number_files": 1, - "size": 4245 + "size": 45336 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:50423ac5123398d8e8b8b283319d07bbf6e5d9c7", - "size": 4245, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-DoubleEG-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:a81eca81", + "size": 45336, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_Charmonium.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30470", + "recid": "30586", "run_period": [ - "Run2016G" + "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016G-DoubleEG-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016H_Charmonium", "type": { "primary": "Supplementaries", "secondary": [ @@ -3764,7 +6414,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3775,7 +6425,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3787,27 +6437,27 @@ "py" ], "number_files": 1, - "size": 4230 + "size": 41863 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:46b1314b12de926e430cd3b19d25297d5e90b598", - "size": 4230, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-MET-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:4ce08280", + "size": 41863, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_DisplacedJet.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30471", + "recid": "30587", "run_period": [ - "Run2016G" + "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016G-MET-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016H_DisplacedJet", "type": { "primary": "Supplementaries", "secondary": [ @@ -3817,7 +6467,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3828,7 +6478,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3840,27 +6490,27 @@ "py" ], "number_files": 1, - "size": 4239 + "size": 41856 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:0ff88e0d5e959d413af203932cabe84e374dd5db", - "size": 4239, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-MuOnia-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:913d7f59", + "size": 41856, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_HTMHT.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30472", + "recid": "30588", "run_period": [ "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016H-MuOnia-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016H_HTMHT", "type": { "primary": "Supplementaries", "secondary": [ @@ -3870,7 +6520,7 @@ }, { "abstract": { - "description": "The configuration file used in NANO data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3881,7 +6531,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3893,27 +6543,27 @@ "py" ], "number_files": 1, - "size": 4251 + "size": 44203 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:b0bbcf5720b136ee3b74f5c5949ffd33760a829d", - "size": 4251, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-DoubleMuon-UL2016_MiniAODv2_NanoAODv9.py" + "checksum": "adler32:58eb6c94", + "size": 44203, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_MuOnia.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30473", + "recid": "30589", "run_period": [ "Run2016H" ], - "title": "Configuration file for NANO step ReReco-Run2016H-DoubleMuon-UL2016_MiniAODv2_NanoAODv9", + "title": "Configuration file for RECO step recoskim_Run2016H_MuOnia", "type": { "primary": "Supplementaries", "secondary": [ @@ -3923,7 +6573,7 @@ }, { "abstract": { - "description": "The configuration file used in PAT data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3934,7 +6584,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3946,27 +6596,27 @@ "py" ], "number_files": 1, - "size": 10017 + "size": 69594 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:c247d38eddd392802db75fe00134585eede453d8", - "size": 10017, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-Charmonium-UL2016_MiniAODv2.py" + "checksum": "adler32:8c20b67c", + "size": 69594, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_MuonEG.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30474", + "recid": "30590", "run_period": [ - "Run2016G" + "Run2016H" ], - "title": "Configuration file for PAT step ReReco-Run2016G-Charmonium-UL2016_MiniAODv2", + "title": "Configuration file for RECO step recoskim_Run2016H_MuonEG", "type": { "primary": "Supplementaries", "secondary": [ @@ -3976,7 +6626,7 @@ }, { "abstract": { - "description": "The configuration file used in PAT data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -3987,7 +6637,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -3999,27 +6649,27 @@ "py" ], "number_files": 1, - "size": 9912 + "size": 95212 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:8434b01136c978719f07ba93b4baf79eb0a28c01", - "size": 9912, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-DisplacedJet-UL2016_MiniAODv2.py" + "checksum": "adler32:190bcf9f", + "size": 95212, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_SinglePhoton.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30475", + "recid": "30591", "run_period": [ - "Run2016G" + "Run2016H" ], - "title": "Configuration file for PAT step ReReco-Run2016G-DisplacedJet-UL2016_MiniAODv2", + "title": "Configuration file for RECO step recoskim_Run2016H_SinglePhoton", "type": { "primary": "Supplementaries", "secondary": [ @@ -4029,7 +6679,7 @@ }, { "abstract": { - "description": "The configuration file used in PAT data processing step." + "description": "The configuration file used in RECO data processing step." }, "accelerator": "CERN-LHC", "collaboration": { @@ -4040,7 +6690,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -4052,27 +6702,27 @@ "py" ], "number_files": 1, - "size": 9912 + "size": 41854 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:565d6448ed9b7e4e5e41512c7ec0d35355942b88", - "size": 9912, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-DisplacedJet-UL2016_MiniAODv2.py" + "checksum": "adler32:a5667efe", + "size": 41854, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/recoskim_Run2016H_Tau.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30476", + "recid": "30592", "run_period": [ "Run2016H" ], - "title": "Configuration file for PAT step ReReco-Run2016H-DisplacedJet-UL2016_MiniAODv2", + "title": "Configuration file for RECO step recoskim_Run2016H_Tau", "type": { "primary": "Supplementaries", "secondary": [ @@ -4093,7 +6743,7 @@ "CMS-Configuration-Files" ], "collision_information": { - "energy": "13Tev", + "energy": "13TeV", "type": "pp" }, "date_created": [ @@ -4105,27 +6755,27 @@ "py" ], "number_files": 1, - "size": 9894 + "size": 11124 }, "experiment": [ "CMS" ], "files": [ { - "checksum": "adler32:4abdc79ff72e86e886e38c2a931d2ca229e6152f", - "size": 9894, - "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016G-MuOnia-UL2016_MiniAODv2.py" + "checksum": "adler32:841240d", + "size": 11124, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/configuration-files/2016/ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2_BParking.py" } ], "note": { "description": "This file describes the exact setup for the CMS software executable which was used in a data-processing step. It is provided only for information purposes. Although all the components required to analyse the public primary datasets - such as corresponding input data, condition data, software version - are provided on this portal, it is not necessarily possible to reproduce all the described data-processing steps." }, "publisher": "CERN Open Data Portal", - "recid": "30477", + "recid": "30593", "run_period": [ - "Run2016G" + "Run2016H" ], - "title": "Configuration file for PAT step ReReco-Run2016G-MuOnia-UL2016_MiniAODv2", + "title": "Configuration file for PAT step ReReco-Run2016H-SingleElectron-UL2016_MiniAODv2_BParking", "type": { "primary": "Supplementaries", "secondary": [ diff --git a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_03.json b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_03.json index 7358de5d4b..bba881565d 100644 --- a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_03.json +++ b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_03.json @@ -22570,6 +22570,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.021e+02", + "total_value_uncertainty": "1.508e-01" + }, "date_created": [ "2015" ], @@ -22771,6 +22778,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.308e+01", + "total_value_uncertainty": "5.477e-02" + }, "date_created": [ "2015" ], @@ -23022,6 +23036,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.278e+01", + "total_value_uncertainty": "3.390e-02" + }, "date_created": [ "2015" ], @@ -23279,6 +23300,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.343e+02", + "total_value_uncertainty": "2.853e-01" + }, "date_created": [ "2015" ], @@ -92767,6 +92795,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.318e+02", + "total_value_uncertainty": "7.360e-01" + }, "date_created": [ "2015" ], @@ -93053,6 +93088,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.012e+03", + "total_value_uncertainty": "2.733e-01" + }, "date_created": [ "2015" ], @@ -93283,6 +93325,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.048e+02", + "total_value_uncertainty": "1.182e+00" + }, "date_created": [ "2015" ], @@ -93541,6 +93590,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.343e+02", + "total_value_uncertainty": "9.842e-02" + }, "date_created": [ "2015" ], @@ -93785,6 +93841,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.022e+02", + "total_value_uncertainty": "4.151e-02" + }, "date_created": [ "2015" ], @@ -94001,6 +94064,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.446e+01", + "total_value_uncertainty": "2.603e-02" + }, "date_created": [ "2015" ], @@ -94217,6 +94287,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.156e+01", + "total_value_uncertainty": "7.092e-03" + }, "date_created": [ "2015" ], @@ -94503,6 +94580,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.009e+01", + "total_value_uncertainty": "5.434e-02" + }, "date_created": [ "2015" ], @@ -94747,6 +94831,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.874e+01", + "total_value_uncertainty": "4.503e-02" + }, "date_created": [ "2015" ], @@ -94963,6 +95054,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.551e+02", + "total_value_uncertainty": "1.271e-01" + }, "date_created": [ "2015" ], @@ -95235,6 +95333,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.633e-02", + "total_value_uncertainty": "6.737e-05" + }, "date_created": [ "2015" ], @@ -95465,6 +95570,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.620e-02", + "total_value_uncertainty": "3.055e-04" + }, "date_created": [ "2015" ], @@ -95681,6 +95793,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.277e+02", + "total_value_uncertainty": "4.544e-01" + }, "date_created": [ "2015" ], @@ -95897,6 +96016,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.276e+02", + "total_value_uncertainty": "9.861e-01" + }, "date_created": [ "2015" ], @@ -96113,6 +96239,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.877e+04", + "total_value_uncertainty": "3.259e+01" + }, "date_created": [ "2015" ], @@ -96385,6 +96518,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.876e+04", + "total_value_uncertainty": "3.258e+01" + }, "date_created": [ "2015" ], @@ -96578,6 +96718,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.877e+04", + "total_value_uncertainty": "3.260e+01" + }, "date_created": [ "2015" ], @@ -96864,6 +97011,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.178e-03", + "total_value_uncertainty": "9.717e-06" + }, "date_created": [ "2015" ], @@ -97094,6 +97248,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.234e-03", + "total_value_uncertainty": "4.445e-05" + }, "date_created": [ "2015" ], @@ -97310,6 +97471,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.652e+00", + "total_value_uncertainty": "2.344e-03" + }, "date_created": [ "2015" ], @@ -97596,6 +97764,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.201e-04", + "total_value_uncertainty": "2.535e-06" + }, "date_created": [ "2015" ], @@ -97826,6 +98001,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.086e-04", + "total_value_uncertainty": "1.174e-05" + }, "date_created": [ "2015" ], @@ -98042,6 +98224,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.724e+00", + "total_value_uncertainty": "1.729e-02" + }, "date_created": [ "2015" ], @@ -98272,6 +98461,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.743e+00", + "total_value_uncertainty": "2.431e-02" + }, "date_created": [ "2015" ], @@ -98502,6 +98698,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.713e+00", + "total_value_uncertainty": "1.176e-01" + }, "date_created": [ "2015" ], @@ -98718,6 +98921,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.064e-01", + "total_value_uncertainty": "1.428e-03" + }, "date_created": [ "2015" ], @@ -98934,6 +99144,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.087e-01", + "total_value_uncertainty": "6.373e-03" + }, "date_created": [ "2015" ], @@ -99150,6 +99367,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.321e-01", + "total_value_uncertainty": "8.431e-04" + }, "date_created": [ "2015" ], @@ -99366,6 +99590,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.346e-01", + "total_value_uncertainty": "3.868e-03" + }, "date_created": [ "2015" ], @@ -99582,6 +99813,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.488e+02", + "total_value_uncertainty": "4.884e-02" + }, "date_created": [ "2015" ], @@ -99798,6 +100036,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.475e+02", + "total_value_uncertainty": "8.589e-02" + }, "date_created": [ "2015" ], @@ -100028,6 +100273,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.511e-01", + "total_value_uncertainty": "1.855e-04" + }, "date_created": [ "2015" ], @@ -100272,6 +100524,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.093e+01", + "total_value_uncertainty": "1.386e-02" + }, "date_created": [ "2015" ], @@ -100488,6 +100747,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.104e+01", + "total_value_uncertainty": "4.009e-02" + }, "date_created": [ "2015" ], @@ -100704,6 +100970,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.658e-03", + "total_value_uncertainty": "5.618e-06" + }, "date_created": [ "2015" ], @@ -100948,6 +101221,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.684e+00", + "total_value_uncertainty": "1.822e-03" + }, "date_created": [ "2015" ], @@ -101206,6 +101486,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.675e+00", + "total_value_uncertainty": "5.277e-03" + }, "date_created": [ "2015" ], @@ -101422,6 +101709,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.360e+00", + "total_value_uncertainty": "4.558e-04" + }, "date_created": [ "2015" ], @@ -101666,6 +101960,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.198e+00", + "total_value_uncertainty": "1.050e-03" + }, "date_created": [ "2015" ], @@ -101882,6 +102183,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.200e+00", + "total_value_uncertainty": "2.085e-03" + }, "date_created": [ "2015" ], @@ -102098,6 +102406,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.236e-01", + "total_value_uncertainty": "3.680e-04" + }, "date_created": [ "2015" ], @@ -102370,6 +102685,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.942e+01", + "total_value_uncertainty": "1.723e-01" + }, "date_created": [ "2015" ], @@ -102586,6 +102908,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.933e+03", + "total_value_uncertainty": "9.220e+00" + }, "date_created": [ "2015" ], @@ -102872,6 +103201,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.932e+03", + "total_value_uncertainty": "9.217e+00" + }, "date_created": [ "2015" ], @@ -103093,6 +103429,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.932e+03", + "total_value_uncertainty": "9.217e+00" + }, "date_created": [ "2015" ], @@ -103379,6 +103722,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.934e+03", + "total_value_uncertainty": "9.221e+00" + }, "date_created": [ "2015" ], @@ -103623,6 +103973,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.958e+03", + "total_value_uncertainty": "2.823e+00" + }, "date_created": [ "2015" ], @@ -103853,6 +104210,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.958e+03", + "total_value_uncertainty": "2.826e+00" + }, "date_created": [ "2015" ], @@ -104125,6 +104489,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.955e+03", + "total_value_uncertainty": "1.268e+00" + }, "date_created": [ "2015" ], @@ -104439,6 +104810,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.954e+03", + "total_value_uncertainty": "1.336e+00" + }, "date_created": [ "2015" ], @@ -104655,6 +105033,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.954e+03", + "total_value_uncertainty": "1.348e+00" + }, "date_created": [ "2015" ], @@ -104927,6 +105312,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.835e+01", + "total_value_uncertainty": "1.154e-02" + }, "date_created": [ "2015" ], @@ -105143,6 +105535,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.234e+02", + "total_value_uncertainty": "7.203e-02" + }, "date_created": [ "2015" ], @@ -105401,6 +105800,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.241e+02", + "total_value_uncertainty": "2.075e-01" + }, "date_created": [ "2015" ], @@ -105617,6 +106023,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.783e+01", + "total_value_uncertainty": "2.524e-02" + }, "date_created": [ "2015" ], @@ -105889,6 +106302,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.788e+01", + "total_value_uncertainty": "3.548e-02" + }, "date_created": [ "2015" ], @@ -106105,6 +106525,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.641e+00", + "total_value_uncertainty": "2.474e-03" + }, "date_created": [ "2015" ], @@ -106363,6 +106790,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.643e+00", + "total_value_uncertainty": "3.461e-03" + }, "date_created": [ "2015" ], @@ -106593,6 +107027,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.099e+00", + "total_value_uncertainty": "7.598e-04" + }, "date_created": [ "2015" ], @@ -106865,6 +107306,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.099e+00", + "total_value_uncertainty": "1.045e-03" + }, "date_created": [ "2015" ], @@ -107081,6 +107529,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.119e+04", + "total_value_uncertainty": "1.067e+01" + }, "date_created": [ "2015" ], @@ -107353,6 +107808,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.594e-02", + "total_value_uncertainty": "1.388e-04" + }, "date_created": [ "2015" ], @@ -107569,6 +108031,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.499e-02", + "total_value_uncertainty": "5.924e-04" + }, "date_created": [ "2015" ], @@ -107799,6 +108268,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.058e-02", + "total_value_uncertainty": "1.212e-04" + }, "date_created": [ "2015" ], @@ -108029,6 +108505,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.106e-02", + "total_value_uncertainty": "5.517e-04" + }, "date_created": [ "2015" ], @@ -108245,6 +108728,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.649e+01", + "total_value_uncertainty": "4.173e-02" + }, "date_created": [ "2015" ], @@ -108475,6 +108965,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.734e+03", + "total_value_uncertainty": "7.447e+00" + }, "date_created": [ "2015" ], @@ -108719,6 +109216,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.208e+03", + "total_value_uncertainty": "3.608e-01" + }, "date_created": [ "2015" ], @@ -108949,6 +109453,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.989e+03", + "total_value_uncertainty": "4.028e+00" + }, "date_created": [ "2015" ], diff --git a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_04.json b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_04.json index ec5d8a0d0a..b34d36b231 100644 --- a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_04.json +++ b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_04.json @@ -22,6 +22,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.988e+03", + "total_value_uncertainty": "3.506e+00" + }, "date_created": [ "2015" ], @@ -308,6 +315,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -572,6 +586,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.409e+02", + "total_value_uncertainty": "3.505e-01" + }, "date_created": [ "2015" ], @@ -872,6 +893,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.964e+04", + "total_value_uncertainty": "1.443e+01" + }, "date_created": [ "2015" ], @@ -1059,6 +1087,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.172e+01", + "total_value_uncertainty": "3.264e-03" + }, "date_created": [ "2015" ], @@ -1260,6 +1295,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.998e-02", + "total_value_uncertainty": "1.823e-05" + }, "date_created": [ "2015" ], @@ -1447,6 +1489,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.579e-04", + "total_value_uncertainty": "3.479e-07" + }, "date_created": [ "2015" ], @@ -5308,6 +5357,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.035e+01", + "total_value_uncertainty": "1.822e-03" + }, "date_created": [ "2015" ], @@ -5524,6 +5580,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.581e+01", + "total_value_uncertainty": "3.580e-03" + }, "date_created": [ "2015" ], @@ -5740,6 +5803,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.997e+00", + "total_value_uncertainty": "6.508e-04" + }, "date_created": [ "2015" ], @@ -5956,6 +6026,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "1.0", + "neg_weight_fraction": "0.000e+00", + "total_value": "1.003e+01", + "total_value_uncertainty": "2.024e-03" + }, "date_created": [ "2015" ], @@ -12412,6 +12489,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.150e-02", + "total_value_uncertainty": "2.101e-05" + }, "date_created": [ "2015" ], @@ -12593,6 +12677,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.157e-02", + "total_value_uncertainty": "2.116e-05" + }, "date_created": [ "2015" ], @@ -12794,6 +12885,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.954e-04", + "total_value_uncertainty": "1.007e-06" + }, "date_created": [ "2015" ], @@ -13017,6 +13115,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.887e-04", + "total_value_uncertainty": "9.855e-07" + }, "date_created": [ "2015" ], @@ -13204,6 +13309,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.229e+00", + "total_value_uncertainty": "2.012e-03" + }, "date_created": [ "2015" ], @@ -13399,6 +13511,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.248e+00", + "total_value_uncertainty": "2.059e-03" + }, "date_created": [ "2015" ], @@ -13600,6 +13719,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.383e-06", + "total_value_uncertainty": "6.039e-09" + }, "date_created": [ "2015" ], @@ -13795,6 +13921,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.442e-06", + "total_value_uncertainty": "6.246e-09" + }, "date_created": [ "2015" ], @@ -14024,6 +14157,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.478e-01", + "total_value_uncertainty": "2.130e-04" + }, "date_created": [ "2015" ], @@ -14233,6 +14373,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.475e-01", + "total_value_uncertainty": "2.126e-04" + }, "date_created": [ "2015" ], @@ -14462,6 +14609,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.916e-08", + "total_value_uncertainty": "5.442e-11" + }, "date_created": [ "2015" ], @@ -14657,6 +14811,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.926e-08", + "total_value_uncertainty": "5.450e-11" + }, "date_created": [ "2015" ], @@ -14886,6 +15047,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.813e+00", + "total_value_uncertainty": "8.123e-03" + }, "date_created": [ "2015" ], @@ -15067,6 +15235,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.796e+00", + "total_value_uncertainty": "7.843e-03" + }, "date_created": [ "2015" ], @@ -15254,6 +15429,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.191e-11", + "total_value_uncertainty": "2.296e-13" + }, "date_created": [ "2015" ], @@ -15435,6 +15617,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.310e-11", + "total_value_uncertainty": "2.330e-13" + }, "date_created": [ "2015" ], @@ -15622,6 +15811,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.292e-03", + "total_value_uncertainty": "1.322e-05" + }, "date_created": [ "2015" ], @@ -15966,6 +16162,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.923e-01", + "total_value_uncertainty": "2.159e-03" + }, "date_created": [ "2015" ], @@ -16153,6 +16356,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.669e-06", + "total_value_uncertainty": "5.247e-09" + }, "date_created": [ "2015" ], @@ -16354,6 +16564,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.592e-02", + "total_value_uncertainty": "1.814e-04" + }, "date_created": [ "2015" ], @@ -16541,6 +16758,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.430e-11", + "total_value_uncertainty": "5.430e-11" + }, "date_created": [ "2015" ], @@ -21070,6 +21294,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.389e+02", + "total_value_uncertainty": "1.345e+00" + }, "date_created": [ "2015" ], @@ -21257,6 +21488,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.659e+05", + "total_value_uncertainty": "5.432e+01" + }, "date_created": [ "2015" ], @@ -21458,6 +21696,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.658e+05", + "total_value_uncertainty": "1.309e+02" + }, "date_created": [ "2015" ], @@ -21645,6 +21890,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.590e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.189e+02", + "total_value_uncertainty": "1.790e-01" + }, "date_created": [ "2015" ], @@ -21854,6 +22106,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.590e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.189e+02", + "total_value_uncertainty": "6.917e-02" + }, "date_created": [ "2015" ], @@ -22097,6 +22356,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.099e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.241e+03", + "total_value_uncertainty": "1.017e+00" + }, "date_created": [ "2015" ], @@ -22340,6 +22606,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "5.137e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.626e+02", + "total_value_uncertainty": "4.251e-01" + }, "date_created": [ "2015" ], @@ -22591,6 +22864,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "5.134e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.621e+02", + "total_value_uncertainty": "2.674e-01" + }, "date_created": [ "2015" ], @@ -22834,6 +23114,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.863e+03", + "total_value_uncertainty": "1.445e+00" + }, "date_created": [ "2015" ], @@ -23078,6 +23365,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.082e+03", + "total_value_uncertainty": "3.257e-01" + }, "date_created": [ "2015" ], @@ -23336,6 +23630,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.271e+02", + "total_value_uncertainty": "3.848e-02" + }, "date_created": [ "2015" ], @@ -23608,6 +23909,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.840e+04", + "total_value_uncertainty": "5.217e+00" + }, "date_created": [ "2015" ], @@ -23866,6 +24174,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.356e+01", + "total_value_uncertainty": "1.323e-02" + }, "date_created": [ "2015" ], @@ -24096,6 +24411,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.234e+03", + "total_value_uncertainty": "3.811e+00" + }, "date_created": [ "2015" ], @@ -24354,6 +24676,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.303e+03", + "total_value_uncertainty": "6.896e-01" + }, "date_created": [ "2015" ], @@ -24598,6 +24927,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.745e+02", + "total_value_uncertainty": "1.690e-01" + }, "date_created": [ "2015" ], @@ -24828,6 +25164,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.081e+04", + "total_value_uncertainty": "9.024e+00" + }, "date_created": [ "2015" ], @@ -25072,6 +25415,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.351e+01", + "total_value_uncertainty": "5.721e-02" + }, "date_created": [ "2015" ], diff --git a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_05.json b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_05.json index 76562a0384..ebbb0b0749 100644 --- a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_05.json +++ b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_05.json @@ -88098,6 +88098,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.337e+01", + "total_value_uncertainty": "1.499e-01" + }, "date_created": [ "2015" ], diff --git a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_07.json b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_07.json index ec36d8a536..6e199ebadf 100644 --- a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_07.json +++ b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_07.json @@ -32823,6 +32823,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "4.619e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.622e+08", + "total_value_uncertainty": "1.176e+05" + }, "date_created": [ "2015" ], @@ -33024,6 +33031,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "4.618e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.622e+08", + "total_value_uncertainty": "1.165e+05" + }, "date_created": [ "2015" ], @@ -33211,6 +33225,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "3.736e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.221e+08", + "total_value_uncertainty": "1.054e+05" + }, "date_created": [ "2015" ], @@ -33454,6 +33475,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.113e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.657e+08", + "total_value_uncertainty": "1.019e+05" + }, "date_created": [ "2015" ], @@ -33697,6 +33725,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.113e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.657e+08", + "total_value_uncertainty": "1.021e+05" + }, "date_created": [ "2015" ], @@ -33926,6 +33961,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.463e+04", + "total_value_uncertainty": "1.111e+01" + }, "date_created": [ "2015" ], @@ -34155,6 +34197,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.338e+12", + "total_value_uncertainty": "3.907e+08" + }, "date_created": [ "2015" ], @@ -38030,6 +38079,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.171e+01", + "total_value_uncertainty": "3.232e-03" + }, "date_created": [ "2015" ], @@ -38245,6 +38301,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.994e-02", + "total_value_uncertainty": "2.282e-05" + }, "date_created": [ "2015" ], @@ -38432,6 +38495,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.578e-04", + "total_value_uncertainty": "3.879e-07" + }, "date_created": [ "2015" ], @@ -43071,6 +43141,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.212e+01", + "total_value_uncertainty": "3.132e-01" + }, "date_created": [ "2015" ], @@ -43258,6 +43335,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.511e-02", + "total_value_uncertainty": "8.298e-05" + }, "date_created": [ "2015" ], @@ -43445,6 +43529,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.139e+00", + "total_value_uncertainty": "2.193e-02" + }, "date_created": [ "2015" ], @@ -43632,6 +43723,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.269e+01", + "total_value_uncertainty": "3.161e-01" + }, "date_created": [ "2015" ], @@ -43833,6 +43931,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.520e-02", + "total_value_uncertainty": "8.386e-05" + }, "date_created": [ "2015" ], @@ -44034,6 +44139,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.162e+00", + "total_value_uncertainty": "2.180e-02" + }, "date_created": [ "2015" ], @@ -54011,6 +54123,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.079e+08", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -54198,6 +54317,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.161e+01", + "total_value_uncertainty": "1.053e-01" + }, "date_created": [ "2015" ], @@ -54414,6 +54540,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.312e+06", + "total_value_uncertainty": "5.260e+02" + }, "date_created": [ "2015" ], @@ -54672,6 +54805,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.447e+00", + "total_value_uncertainty": "1.879e-02" + }, "date_created": [ "2015" ], @@ -54888,6 +55028,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.847e-01", + "total_value_uncertainty": "4.879e-03" + }, "date_created": [ "2015" ], @@ -55132,6 +55279,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.825e+04", + "total_value_uncertainty": "3.841e+01" + }, "date_created": [ "2015" ], @@ -55432,6 +55586,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.797e+04", + "total_value_uncertainty": "1.012e+01" + }, "date_created": [ "2015" ], @@ -55690,6 +55851,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.596e+03", + "total_value_uncertainty": "1.009e+00" + }, "date_created": [ "2015" ], @@ -55906,6 +56074,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.214e+02", + "total_value_uncertainty": "3.301e-01" + }, "date_created": [ "2015" ], @@ -56136,6 +56311,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.116e+08", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -56323,6 +56505,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.119e+08", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -56510,6 +56699,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.894e+02", + "total_value_uncertainty": "1.675e-01" + }, "date_created": [ "2015" ], @@ -56737,6 +56933,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "5.167e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.238e+02", + "total_value_uncertainty": "2.366e-01" + }, "date_created": [ "2015" ], @@ -57009,6 +57212,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.208e+03", + "total_value_uncertainty": "3.691e-01" + }, "date_created": [ "2015" ], @@ -57281,6 +57491,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.208e+03", + "total_value_uncertainty": "5.194e-01" + }, "date_created": [ "2015" ], @@ -57525,6 +57742,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.863e+06", + "total_value_uncertainty": "6.169e+02" + }, "date_created": [ "2015" ], @@ -57780,6 +58004,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.799e+07", + "total_value_uncertainty": "8.242e+03" + }, "date_created": [ "2015" ], @@ -58066,6 +58297,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.035e+01", + "total_value_uncertainty": "3.256e-02" + }, "date_created": [ "2015" ], @@ -58279,6 +58517,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "5.602e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.718e+01", + "total_value_uncertainty": "4.667e-02" + }, "date_created": [ "2015" ], @@ -58523,6 +58768,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.199e+02", + "total_value_uncertainty": "4.145e-02" + }, "date_created": [ "2015" ], @@ -58781,6 +59033,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.201e+02", + "total_value_uncertainty": "5.847e-02" + }, "date_created": [ "2015" ], @@ -58997,6 +59256,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.463e+00", + "total_value_uncertainty": "9.337e-03" + }, "date_created": [ "2015" ], @@ -59252,6 +59518,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "5.710e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.446e+01", + "total_value_uncertainty": "1.850e-02" + }, "date_created": [ "2015" ], @@ -59482,6 +59755,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.534e+01", + "total_value_uncertainty": "1.220e-02" + }, "date_created": [ "2015" ], @@ -59740,6 +60020,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.527e+01", + "total_value_uncertainty": "1.732e-02" + }, "date_created": [ "2015" ], @@ -59970,6 +60257,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.543e+05", + "total_value_uncertainty": "4.762e+01" + }, "date_created": [ "2015" ], @@ -60225,6 +60519,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.711e+06", + "total_value_uncertainty": "5.146e+02" + }, "date_created": [ "2015" ], @@ -60497,6 +60798,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.712e+06", + "total_value_uncertainty": "5.148e+02" + }, "date_created": [ "2015" ], @@ -60741,6 +61049,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.774e+04", + "total_value_uncertainty": "1.323e+01" + }, "date_created": [ "2015" ], @@ -60996,6 +61311,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.020e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.026e+04", + "total_value_uncertainty": "2.203e+01" + }, "date_created": [ "2015" ], @@ -61268,6 +61590,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.478e+05", + "total_value_uncertainty": "1.054e+02" + }, "date_created": [ "2015" ], @@ -61540,6 +61869,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.476e+05", + "total_value_uncertainty": "1.053e+02" + }, "date_created": [ "2015" ], @@ -61812,6 +62148,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.153e+03", + "total_value_uncertainty": "1.302e+00" + }, "date_created": [ "2015" ], @@ -62067,6 +62410,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "3.512e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.127e+04", + "total_value_uncertainty": "3.519e+00" + }, "date_created": [ "2015" ], @@ -62311,6 +62661,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.209e+04", + "total_value_uncertainty": "9.774e+00" + }, "date_created": [ "2015" ], @@ -62569,6 +62926,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.211e+04", + "total_value_uncertainty": "9.779e+00" + }, "date_created": [ "2015" ], @@ -62813,6 +63177,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.783e+02", + "total_value_uncertainty": "4.734e-01" + }, "date_created": [ "2015" ], @@ -63040,6 +63411,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "4.440e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.035e+03", + "total_value_uncertainty": "9.452e-01" + }, "date_created": [ "2015" ], @@ -63312,6 +63690,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.830e+03", + "total_value_uncertainty": "2.085e+00" + }, "date_created": [ "2015" ], @@ -63584,6 +63969,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.835e+03", + "total_value_uncertainty": "2.086e+00" + }, "date_created": [ "2015" ], @@ -63800,6 +64192,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.977e+09", + "total_value_uncertainty": "7.459e+05" + }, "date_created": [ "2015" ], @@ -63987,6 +64386,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.979e+09", + "total_value_uncertainty": "7.456e+05" + }, "date_created": [ "2015" ], @@ -64174,6 +64580,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.371e+00", + "total_value_uncertainty": "2.584e-03" + }, "date_created": [ "2015" ], @@ -64375,6 +64788,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.555e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.619e+00", + "total_value_uncertainty": "7.666e-04" + }, "date_created": [ "2015" ], @@ -64576,6 +64996,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.867e+09", + "total_value_uncertainty": "1.119e+06" + }, "date_created": [ "2015" ], @@ -64805,6 +65232,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.930e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.940e+08", + "total_value_uncertainty": "1.589e+05" + }, "date_created": [ "2015" ], @@ -65006,6 +65440,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.927e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.938e+08", + "total_value_uncertainty": "2.625e+05" + }, "date_created": [ "2015" ], @@ -65193,6 +65634,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "3.732e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.217e+08", + "total_value_uncertainty": "1.068e+05" + }, "date_created": [ "2015" ], @@ -65380,6 +65828,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.606e+09", + "total_value_uncertainty": "3.711e+06" + }, "date_created": [ "2015" ], @@ -65595,6 +66050,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.750e+09", + "total_value_uncertainty": "3.832e+06" + }, "date_created": [ "2015" ], @@ -65810,6 +66272,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.621e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.605e+04", + "total_value_uncertainty": "2.251e+01" + }, "date_created": [ "2015" ], @@ -66053,6 +66522,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "5.431e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.549e+04", + "total_value_uncertainty": "8.840e+00" + }, "date_created": [ "2015" ], @@ -66310,6 +66786,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.662e+05", + "total_value_uncertainty": "8.737e+01" + }, "date_created": [ "2015" ], @@ -66539,6 +67022,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.376e-01", + "total_value_uncertainty": "6.358e-04" + }, "date_created": [ "2015" ], @@ -66726,6 +67216,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.592e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.841e+08", + "total_value_uncertainty": "1.661e+05" + }, "date_created": [ "2015" ], @@ -66913,6 +67410,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.819e-04", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.318e+05", + "total_value_uncertainty": "1.414e+02" + }, "date_created": [ "2015" ], @@ -67100,6 +67604,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.279e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.629e+06", + "total_value_uncertainty": "6.961e+02" + }, "date_created": [ "2015" ], @@ -67301,6 +67812,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.847e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.626e+06", + "total_value_uncertainty": "1.666e+03" + }, "date_created": [ "2015" ], @@ -67502,6 +68020,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.972e+09", + "total_value_uncertainty": "3.400e+05" + }, "date_created": [ "2015" ], @@ -67689,6 +68214,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.820e+09", + "total_value_uncertainty": "2.944e+05" + }, "date_created": [ "2015" ], @@ -67904,6 +68436,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.976e+09", + "total_value_uncertainty": "3.428e+05" + }, "date_created": [ "2015" ], @@ -68119,6 +68658,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.976e+09", + "total_value_uncertainty": "3.338e+05" + }, "date_created": [ "2015" ], @@ -68348,6 +68894,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.024e+10", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -68605,6 +69158,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.466e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.608e+03", + "total_value_uncertainty": "8.352e-01" + }, "date_created": [ "2015" ], @@ -68820,6 +69380,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.593e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.880e+04", + "total_value_uncertainty": "5.572e+00" + }, "date_created": [ "2015" ], @@ -69021,6 +69588,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "7.312e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.636e+03", + "total_value_uncertainty": "2.984e+00" + }, "date_created": [ "2015" ], @@ -69250,6 +69824,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.172e+05", + "total_value_uncertainty": "2.188e+01" + }, "date_created": [ "2015" ], @@ -69451,6 +70032,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.123e-01", + "total_value_uncertainty": "9.128e-05" + }, "date_created": [ "2015" ], @@ -69638,6 +70226,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "6.509e-04", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.634e+05", + "total_value_uncertainty": "1.149e+02" + }, "date_created": [ "2015" ], @@ -69853,6 +70448,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "9.948e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.555e+06", + "total_value_uncertainty": "1.818e+03" + }, "date_created": [ "2015" ], @@ -70040,6 +70642,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "5.646e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.152e+06", + "total_value_uncertainty": "9.948e+02" + }, "date_created": [ "2015" ], @@ -70283,6 +70892,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "3.738e-04", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.693e+05", + "total_value_uncertainty": "8.516e+01" + }, "date_created": [ "2015" ], @@ -70484,6 +71100,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.742e-03", + "total_value_uncertainty": "5.489e-06" + }, "date_created": [ "2015" ], @@ -70671,6 +71294,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "3.427e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.220e+02", + "total_value_uncertainty": "2.254e-01" + }, "date_created": [ "2015" ], @@ -70872,6 +71502,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.018e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.959e+02", + "total_value_uncertainty": "2.729e-01" + }, "date_created": [ "2015" ], @@ -71101,6 +71738,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.771e+03", + "total_value_uncertainty": "1.757e+00" + }, "date_created": [ "2015" ], @@ -71372,6 +72016,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.761e+03", + "total_value_uncertainty": "1.555e+00" + }, "date_created": [ "2015" ], @@ -71587,6 +72238,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.399e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.216e+03", + "total_value_uncertainty": "4.251e-01" + }, "date_created": [ "2015" ], @@ -71788,6 +72446,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.045e-04", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.210e+04", + "total_value_uncertainty": "1.642e+01" + }, "date_created": [ "2015" ], @@ -72025,6 +72690,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.046e-04", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.211e+04", + "total_value_uncertainty": "6.991e+00" + }, "date_created": [ "2015" ], @@ -72240,6 +72912,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "4.984e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.955e+06", + "total_value_uncertainty": "3.150e+03" + }, "date_created": [ "2015" ], @@ -72441,6 +73120,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.183e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.652e+06", + "total_value_uncertainty": "5.201e+02" + }, "date_created": [ "2015" ], @@ -72642,6 +73328,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.387e+08", + "total_value_uncertainty": "2.242e+04" + }, "date_created": [ "2015" ], @@ -72829,6 +73522,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.626e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.172e+05", + "total_value_uncertainty": "1.318e+02" + }, "date_created": [ "2015" ], @@ -73030,6 +73730,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.523e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.471e+05", + "total_value_uncertainty": "7.810e+01" + }, "date_created": [ "2015" ], @@ -73259,6 +73966,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.623e-04", + "total_value_uncertainty": "1.429e-07" + }, "date_created": [ "2015" ], @@ -73446,6 +74160,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "8.085e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.961e+06", + "total_value_uncertainty": "6.028e+03" + }, "date_created": [ "2015" ], @@ -73661,6 +74382,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.112e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.656e+08", + "total_value_uncertainty": "1.024e+05" + }, "date_created": [ "2015" ], @@ -73848,6 +74576,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.360e+07", + "total_value_uncertainty": "4.011e+04" + }, "date_created": [ "2015" ], @@ -74063,6 +74798,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.983e+07", + "total_value_uncertainty": "4.990e+04" + }, "date_created": [ "2015" ], @@ -74264,6 +75006,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.096e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.135e+05", + "total_value_uncertainty": "7.862e+01" + }, "date_created": [ "2015" ], @@ -74501,6 +75250,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.098e-03", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.136e+05", + "total_value_uncertainty": "3.589e+01" + }, "date_created": [ "2015" ], @@ -74716,6 +75472,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.227e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.920e+01", + "total_value_uncertainty": "3.843e-02" + }, "date_created": [ "2015" ], @@ -74903,6 +75666,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.409e+02", + "total_value_uncertainty": "1.522e-01" + }, "date_created": [ "2015" ], @@ -75104,6 +75874,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.144e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.199e+06", + "total_value_uncertainty": "6.648e+02" + }, "date_created": [ "2015" ], @@ -75347,6 +76124,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.333e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.488e+05", + "total_value_uncertainty": "1.407e+02" + }, "date_created": [ "2015" ], @@ -75618,6 +76402,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.912e+07", + "total_value_uncertainty": "3.066e+03" + }, "date_created": [ "2015" ], @@ -75833,6 +76624,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.083e+10", + "total_value_uncertainty": "1.148e+07" + }, "date_created": [ "2015" ], @@ -76020,6 +76818,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.349e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.526e+01", + "total_value_uncertainty": "1.196e-02" + }, "date_created": [ "2015" ], @@ -76249,6 +77054,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.859e+02", + "total_value_uncertainty": "4.340e-02" + }, "date_created": [ "2015" ], @@ -76464,6 +77276,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.464e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.725e+00", + "total_value_uncertainty": "2.323e-03" + }, "date_created": [ "2015" ], @@ -76651,6 +77470,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.203e+01", + "total_value_uncertainty": "7.549e-03" + }, "date_created": [ "2015" ], @@ -76852,6 +77678,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.511e-01", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.157e+05", + "total_value_uncertainty": "1.239e+02" + }, "date_created": [ "2015" ], @@ -77109,6 +77942,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "3.823e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.052e+05", + "total_value_uncertainty": "3.281e+01" + }, "date_created": [ "2015" ], @@ -77352,6 +78192,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.735e+06", + "total_value_uncertainty": "5.337e+02" + }, "date_created": [ "2015" ], @@ -77553,6 +78400,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.228e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.959e+04", + "total_value_uncertainty": "1.246e+01" + }, "date_created": [ "2015" ], @@ -77754,6 +78608,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.132e+08", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -77955,6 +78816,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.125e+08", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], diff --git a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_10.json b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_10.json index 51fe83e9c3..c606bc8bc9 100644 --- a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_10.json +++ b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_10.json @@ -56435,6 +56435,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.012e+01", + "total_value_uncertainty": "1.334e-02" + }, "date_created": [ "2015" ], @@ -56693,6 +56700,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.365e+00", + "total_value_uncertainty": "4.584e-03" + }, "date_created": [ "2015" ], @@ -56909,6 +56923,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.697e+01", + "total_value_uncertainty": "1.766e-01" + }, "date_created": [ "2015" ], @@ -57153,6 +57174,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.717e+01", + "total_value_uncertainty": "2.545e-01" + }, "date_created": [ "2015" ], @@ -57411,6 +57439,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.717e+01", + "total_value_uncertainty": "2.545e-01" + }, "date_created": [ "2015" ], @@ -57669,6 +57704,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.887e+01", + "total_value_uncertainty": "2.214e-01" + }, "date_created": [ "2015" ], @@ -57885,6 +57927,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.592e+01", + "total_value_uncertainty": "2.263e-01" + }, "date_created": [ "2015" ], @@ -58115,6 +58164,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.717e+01", + "total_value_uncertainty": "2.545e-01" + }, "date_created": [ "2015" ], @@ -58359,6 +58415,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.717e+01", + "total_value_uncertainty": "2.545e-01" + }, "date_created": [ "2015" ], @@ -58603,6 +58666,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.717e+01", + "total_value_uncertainty": "2.545e-01" + }, "date_created": [ "2015" ], @@ -58847,6 +58917,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.717e+01", + "total_value_uncertainty": "2.545e-01" + }, "date_created": [ "2015" ], @@ -59105,6 +59182,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.734e-01", + "total_value_uncertainty": "4.844e-04" + }, "date_created": [ "2015" ], @@ -59321,6 +59405,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -59530,6 +59621,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.530e+01", + "total_value_uncertainty": "1.935e-01" + }, "date_created": [ "2015" ], @@ -59752,6 +59850,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -60003,6 +60108,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.190e+01", + "total_value_uncertainty": "3.388e-01" + }, "date_created": [ "2015" ], @@ -60225,6 +60337,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.623e+01", + "total_value_uncertainty": "5.671e-02" + }, "date_created": [ "2015" ], @@ -60447,6 +60566,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.806e+01", + "total_value_uncertainty": "3.055e-02" + }, "date_created": [ "2015" ], @@ -60669,6 +60795,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.987e+01", + "total_value_uncertainty": "3.206e-02" + }, "date_created": [ "2015" ], @@ -60877,6 +61010,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.635e+01", + "total_value_uncertainty": "2.912e-02" + }, "date_created": [ "2015" ], @@ -61085,6 +61225,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.806e+01", + "total_value_uncertainty": "3.055e-02" + }, "date_created": [ "2015" ], @@ -61293,6 +61440,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.924e+01", + "total_value_uncertainty": "3.294e-02" + }, "date_created": [ "2015" ], @@ -61501,6 +61655,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.724e+01", + "total_value_uncertainty": "2.867e-02" + }, "date_created": [ "2015" ], @@ -61709,6 +61870,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.621e+01", + "total_value_uncertainty": "5.387e-02" + }, "date_created": [ "2015" ], @@ -61917,6 +62085,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.809e+01", + "total_value_uncertainty": "3.050e-02" + }, "date_created": [ "2015" ], @@ -62125,6 +62300,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.990e+01", + "total_value_uncertainty": "3.201e-02" + }, "date_created": [ "2015" ], @@ -62347,6 +62529,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.639e+01", + "total_value_uncertainty": "2.908e-02" + }, "date_created": [ "2015" ], @@ -62555,6 +62744,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.809e+01", + "total_value_uncertainty": "3.050e-02" + }, "date_created": [ "2015" ], @@ -62763,6 +62959,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.928e+01", + "total_value_uncertainty": "3.294e-02" + }, "date_created": [ "2015" ], @@ -62985,6 +63188,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.728e+01", + "total_value_uncertainty": "2.864e-02" + }, "date_created": [ "2015" ], @@ -86135,6 +86345,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.015e-01", + "total_value_uncertainty": "5.229e-06" + }, "date_created": [ "2015" ], @@ -86351,6 +86568,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.551e+00", + "total_value_uncertainty": "6.630e-05" + }, "date_created": [ "2015" ], @@ -86567,6 +86791,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.967e+00", + "total_value_uncertainty": "1.052e-02" + }, "date_created": [ "2015" ], @@ -86784,6 +87015,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.967e+00", + "total_value_uncertainty": "1.052e-02" + }, "date_created": [ "2015" ], @@ -87001,6 +87239,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.849e+01", + "total_value_uncertainty": "1.724e-02" + }, "date_created": [ "2015" ], @@ -87209,6 +87454,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.166e+01", + "total_value_uncertainty": "3.997e-02" + }, "date_created": [ "2015" ], diff --git a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_11.json b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_11.json index 7542e3f397..43465ca0a7 100644 --- a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_11.json +++ b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_11.json @@ -39205,6 +39205,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.393e+01", + "total_value_uncertainty": "3.629e-02" + }, "date_created": [ "2015" ], @@ -39423,6 +39430,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.393e+01", + "total_value_uncertainty": "3.629e-02" + }, "date_created": [ "2015" ], @@ -39655,6 +39669,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.982e+00", + "total_value_uncertainty": "1.592e-05" + }, "date_created": [ "2015" ], @@ -39927,6 +39948,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.731e-02", + "total_value_uncertainty": "3.715e-05" + }, "date_created": [ "2015" ], @@ -40144,6 +40172,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.772e+00", + "total_value_uncertainty": "9.506e-03" + }, "date_created": [ "2015" ], @@ -55982,6 +56017,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.668e+02", + "total_value_uncertainty": "2.018e+00" + }, "date_created": [ "2015" ], @@ -56231,6 +56273,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.674e+01", + "total_value_uncertainty": "1.569e-02" + }, "date_created": [ "2015" ], @@ -56503,6 +56552,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.685e+01", + "total_value_uncertainty": "2.012e-02" + }, "date_created": [ "2015" ], @@ -56719,6 +56775,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.192e-01", + "total_value_uncertainty": "6.320e-05" + }, "date_created": [ "2015" ], @@ -57005,6 +57068,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.190e-01", + "total_value_uncertainty": "1.076e-04" + }, "date_created": [ "2015" ], @@ -57235,6 +57305,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.446e-03", + "total_value_uncertainty": "1.012e-06" + }, "date_created": [ "2015" ], @@ -57465,6 +57542,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.444e-03", + "total_value_uncertainty": "1.724e-06" + }, "date_created": [ "2015" ], @@ -57681,6 +57765,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.651e+00", + "total_value_uncertainty": "4.830e-04" + }, "date_created": [ "2015" ], @@ -57953,6 +58044,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.652e+00", + "total_value_uncertainty": "6.722e-04" + }, "date_created": [ "2015" ], @@ -58183,6 +58281,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.737e-01", + "total_value_uncertainty": "1.956e-04" + }, "date_created": [ "2015" ], @@ -58399,6 +58504,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.724e-01", + "total_value_uncertainty": "3.274e-04" + }, "date_created": [ "2015" ], @@ -58615,6 +58727,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.305e+02", + "total_value_uncertainty": "2.138e+00" + }, "date_created": [ "2015" ], @@ -58887,6 +59006,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.185e+02", + "total_value_uncertainty": "1.839e+00" + }, "date_created": [ "2015" ], @@ -59131,6 +59257,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.455e+01", + "total_value_uncertainty": "5.999e-02" + }, "date_created": [ "2015" ], @@ -59347,6 +59480,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.141e+02", + "total_value_uncertainty": "3.153e-02" + }, "date_created": [ "2015" ], @@ -59633,6 +59773,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.139e+02", + "total_value_uncertainty": "3.149e-02" + }, "date_created": [ "2015" ], @@ -59849,6 +59996,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.140e+02", + "total_value_uncertainty": "3.151e-02" + }, "date_created": [ "2015" ], @@ -60135,6 +60289,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.140e+02", + "total_value_uncertainty": "3.151e-02" + }, "date_created": [ "2015" ], @@ -60379,6 +60540,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.670e+02", + "total_value_uncertainty": "2.019e+00" + }, "date_created": [ "2015" ], @@ -60651,6 +60819,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.733e+02", + "total_value_uncertainty": "5.685e+00" + }, "date_created": [ "2015" ], @@ -60867,6 +61042,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.181e+02", + "total_value_uncertainty": "1.875e+00" + }, "date_created": [ "2015" ], @@ -61153,6 +61335,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.105e+02", + "total_value_uncertainty": "2.147e+00" + }, "date_created": [ "2015" ], @@ -61425,6 +61614,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.098e+02", + "total_value_uncertainty": "1.411e-01" + }, "date_created": [ "2015" ], @@ -61669,6 +61865,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.576e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.880e+01", + "total_value_uncertainty": "2.201e-02" + }, "date_created": [ "2015" ], @@ -61877,6 +62080,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "2.575e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.879e+01", + "total_value_uncertainty": "1.803e-02" + }, "date_created": [ "2015" ], @@ -62113,6 +62323,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "9.710e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.088e+01", + "total_value_uncertainty": "7.487e-02" + }, "date_created": [ "2015" ], @@ -62321,6 +62538,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "9.703e-02", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.083e+01", + "total_value_uncertainty": "6.770e-02" + }, "date_created": [ "2015" ], @@ -62599,6 +62823,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.669e+01", + "total_value_uncertainty": "7.100e-02" + }, "date_created": [ "2015" ], @@ -62850,6 +63081,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.669e+01", + "total_value_uncertainty": "7.100e-02" + }, "date_created": [ "2015" ], @@ -63086,6 +63324,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.669e+01", + "total_value_uncertainty": "7.100e-02" + }, "date_created": [ "2015" ], @@ -63295,6 +63540,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.669e+01", + "total_value_uncertainty": "7.100e-02" + }, "date_created": [ "2015" ], @@ -63560,6 +63812,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.663e+01", + "total_value_uncertainty": "6.953e-02" + }, "date_created": [ "2015" ], @@ -63768,6 +64027,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.663e+01", + "total_value_uncertainty": "6.953e-02" + }, "date_created": [ "2015" ], @@ -63976,6 +64242,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.663e+01", + "total_value_uncertainty": "6.953e-02" + }, "date_created": [ "2015" ], @@ -64184,6 +64457,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.663e+01", + "total_value_uncertainty": "6.953e-02" + }, "date_created": [ "2015" ], @@ -64392,6 +64672,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -64755,6 +65042,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -65020,6 +65314,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -65271,6 +65572,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.103e-03", + "total_value_uncertainty": "1.401e-05" + }, "date_created": [ "2015" ], @@ -65501,6 +65809,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.103e-03", + "total_value_uncertainty": "1.401e-05" + }, "date_created": [ "2015" ], @@ -65717,6 +66032,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.791e+02", + "total_value_uncertainty": "1.142e+00" + }, "date_created": [ "2015" ], @@ -65948,6 +66270,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.791e+02", + "total_value_uncertainty": "1.142e+00" + }, "date_created": [ "2015" ], @@ -66207,6 +66536,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -66485,6 +66821,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -66777,6 +67120,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -67083,6 +67433,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -67347,6 +67704,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -67555,6 +67919,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -67805,6 +68176,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -68027,6 +68405,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -68333,6 +68718,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -68541,6 +68933,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -68749,6 +69148,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -68985,6 +69391,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -69235,6 +69648,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -69485,6 +69905,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -69721,6 +70148,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -69957,6 +70391,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -70221,6 +70662,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -70513,6 +70961,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -70735,6 +71190,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -70999,6 +71461,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.764e+02", + "total_value_uncertainty": "8.701e-01" + }, "date_created": [ "2015" ], @@ -71230,6 +71699,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -71438,6 +71914,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.300e+02", + "total_value_uncertainty": "6.623e-01" + }, "date_created": [ "2015" ], @@ -71702,6 +72185,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.873e-01", + "total_value_uncertainty": "1.346e-04" + }, "date_created": [ "2015" ], @@ -71918,6 +72408,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.010e-01", + "total_value_uncertainty": "5.647e-04" + }, "date_created": [ "2015" ], @@ -72135,6 +72632,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.062e-01", + "total_value_uncertainty": "8.105e-04" + }, "date_created": [ "2015" ], @@ -72352,6 +72856,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.181e-01", + "total_value_uncertainty": "1.401e-04" + }, "date_created": [ "2015" ], @@ -72568,6 +73079,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.529e-01", + "total_value_uncertainty": "3.378e-04" + }, "date_created": [ "2015" ], @@ -72784,6 +73302,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.297e-01", + "total_value_uncertainty": "7.941e-04" + }, "date_created": [ "2015" ], @@ -73000,6 +73525,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.580e-02", + "total_value_uncertainty": "1.989e-04" + }, "date_created": [ "2015" ], @@ -73244,6 +73776,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.379e-01", + "total_value_uncertainty": "3.630e-04" + }, "date_created": [ "2015" ], @@ -84737,6 +85276,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.704e+00", + "total_value_uncertainty": "8.038e-03" + }, "date_created": [ "2015" ], diff --git a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_12.json b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_12.json index db67b2e0ea..ce7903a883 100644 --- a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_12.json +++ b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_12.json @@ -1087,6 +1087,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.413e-01", + "total_value_uncertainty": "3.465e-03" + }, "date_created": [ "2015" ], @@ -14598,6 +14605,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.193e+01", + "total_value_uncertainty": "1.719e-02" + }, "date_created": [ "2015" ], @@ -14829,6 +14843,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.635e+03", + "total_value_uncertainty": "2.591e+00" + }, "date_created": [ "2015" ], @@ -15115,6 +15136,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.166e+03", + "total_value_uncertainty": "9.292e-01" + }, "date_created": [ "2015" ], @@ -15387,6 +15415,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.491e+02", + "total_value_uncertainty": "2.908e-01" + }, "date_created": [ "2015" ], @@ -15603,6 +15638,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.947e+02", + "total_value_uncertainty": "1.613e-01" + }, "date_created": [ "2015" ], @@ -15875,6 +15917,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.464e+01", + "total_value_uncertainty": "3.388e-02" + }, "date_created": [ "2015" ], @@ -16091,6 +16140,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.565e-01", + "total_value_uncertainty": "7.882e-04" + }, "date_created": [ "2015" ], @@ -16307,6 +16363,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.663e+00", + "total_value_uncertainty": "2.028e-04" + }, "date_created": [ "2015" ], @@ -17049,6 +17112,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "8.195e-03", + "total_value_uncertainty": "6.571e-06" + }, "date_created": [ "2015" ], @@ -17265,6 +17335,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.124e+02", + "total_value_uncertainty": "7.402e-01" + }, "date_created": [ "2015" ], @@ -17481,6 +17558,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.773e+02", + "total_value_uncertainty": "1.215e-01" + }, "date_created": [ "2015" ], @@ -19264,6 +19348,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.031e+02", + "total_value_uncertainty": "9.370e-02" + }, "date_created": [ "2015" ], @@ -19522,6 +19613,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.346e+03", + "total_value_uncertainty": "4.032e-01" + }, "date_created": [ "2015" ], @@ -19738,6 +19836,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.347e+03", + "total_value_uncertainty": "4.033e-01" + }, "date_created": [ "2015" ], @@ -19982,6 +20087,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.329e+00", + "total_value_uncertainty": "4.934e-04" + }, "date_created": [ "2015" ], @@ -20226,6 +20338,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.328e+00", + "total_value_uncertainty": "2.575e-03" + }, "date_created": [ "2015" ], @@ -20442,6 +20561,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.603e+02", + "total_value_uncertainty": "1.090e-01" + }, "date_created": [ "2015" ], @@ -20658,6 +20784,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.596e+02", + "total_value_uncertainty": "1.546e-01" + }, "date_created": [ "2015" ], @@ -20874,6 +21007,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.209e-02", + "total_value_uncertainty": "2.028e-05" + }, "date_created": [ "2015" ], @@ -21160,6 +21300,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.219e-02", + "total_value_uncertainty": "6.147e-05" + }, "date_created": [ "2015" ], @@ -21376,6 +21523,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.880e+01", + "total_value_uncertainty": "1.990e-02" + }, "date_created": [ "2015" ], @@ -21606,6 +21760,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.889e+01", + "total_value_uncertainty": "3.368e-02" + }, "date_created": [ "2015" ], @@ -21836,6 +21997,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.202e+01", + "total_value_uncertainty": "3.655e-03" + }, "date_created": [ "2015" ], @@ -22108,6 +22276,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.205e+01", + "total_value_uncertainty": "5.968e-03" + }, "date_created": [ "2015" ], @@ -22338,6 +22513,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.880e+01", + "total_value_uncertainty": "1.772e-02" + }, "date_created": [ "2015" ], @@ -22554,6 +22736,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.493e+00", + "total_value_uncertainty": "2.156e-03" + }, "date_created": [ "2015" ], @@ -22770,6 +22959,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.480e+00", + "total_value_uncertainty": "4.210e-03" + }, "date_created": [ "2015" ], @@ -23014,6 +23210,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.044e+04", + "total_value_uncertainty": "1.026e+02" + }, "date_created": [ "2015" ], @@ -23314,6 +23517,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.041e+04", + "total_value_uncertainty": "1.025e+02" + }, "date_created": [ "2015" ], @@ -23577,6 +23787,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.049e+04", + "total_value_uncertainty": "1.027e+02" + }, "date_created": [ "2015" ], @@ -23863,6 +24080,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.033e+04", + "total_value_uncertainty": "1.262e+01" + }, "date_created": [ "2015" ], @@ -24135,6 +24359,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.105e+03", + "total_value_uncertainty": "8.907e-01" + }, "date_created": [ "2015" ], @@ -24421,6 +24652,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.966e+01", + "total_value_uncertainty": "9.489e-02" + }, "date_created": [ "2015" ], @@ -24637,6 +24875,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.055e-01", + "total_value_uncertainty": "3.139e-06" + }, "date_created": [ "2015" ], @@ -24853,6 +25098,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.635e-02", + "total_value_uncertainty": "3.918e-06" + }, "date_created": [ "2015" ], @@ -25069,6 +25321,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.983e-01", + "total_value_uncertainty": "1.661e-06" + }, "date_created": [ "2015" ], @@ -25285,6 +25544,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.948e-01", + "total_value_uncertainty": "9.672e-06" + }, "date_created": [ "2015" ], @@ -34488,6 +34754,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -34722,6 +34995,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -34942,6 +35222,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -35176,6 +35463,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -35424,6 +35718,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "7.868e-03", + "total_value_uncertainty": "7.582e-05" + }, "date_created": [ "2015" ], @@ -44535,6 +44836,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -44727,6 +45035,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -45003,6 +45318,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -45237,6 +45559,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], diff --git a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_13.json b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_13.json index 70c28a1447..bc1fd34176 100644 --- a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_13.json +++ b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_13.json @@ -57161,6 +57161,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.093e-02", + "total_value_uncertainty": "1.937e-04" + }, "date_created": [ "2015" ], @@ -57383,6 +57390,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.002e-02", + "total_value_uncertainty": "6.097e-06" + }, "date_created": [ "2015" ], @@ -57613,6 +57627,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.526e-02", + "total_value_uncertainty": "2.107e-06" + }, "date_created": [ "2015" ], @@ -57829,6 +57850,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.471e-02", + "total_value_uncertainty": "2.712e-06" + }, "date_created": [ "2015" ], @@ -67984,6 +68012,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.276e-02", + "total_value_uncertainty": "7.420e-06" + }, "date_created": [ "2015" ], @@ -68171,6 +68206,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.505e+02", + "total_value_uncertainty": "7.689e-02" + }, "date_created": [ "2015" ], @@ -68358,6 +68400,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.021e-04", + "total_value_uncertainty": "2.336e-07" + }, "date_created": [ "2015" ], @@ -68553,6 +68602,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.021e-04", + "total_value_uncertainty": "2.337e-07" + }, "date_created": [ "2015" ], @@ -68740,6 +68796,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.231e+00", + "total_value_uncertainty": "3.279e-03" + }, "date_created": [ "2015" ], @@ -68927,6 +68990,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.896e-05", + "total_value_uncertainty": "1.675e-08" + }, "date_created": [ "2015" ], @@ -69114,6 +69184,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.679e-06", + "total_value_uncertainty": "1.549e-09" + }, "date_created": [ "2015" ], @@ -69323,6 +69400,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.679e-06", + "total_value_uncertainty": "1.554e-09" + }, "date_created": [ "2015" ], @@ -69524,6 +69608,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.705e-07", + "total_value_uncertainty": "1.577e-10" + }, "date_created": [ "2015" ], @@ -69733,6 +69824,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.705e-07", + "total_value_uncertainty": "1.557e-10" + }, "date_created": [ "2015" ], @@ -69934,6 +70032,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.135e-01", + "total_value_uncertainty": "1.194e-04" + }, "date_created": [ "2015" ], @@ -70121,6 +70226,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.789e-08", + "total_value_uncertainty": "1.620e-11" + }, "date_created": [ "2015" ], @@ -70344,6 +70456,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.789e-08", + "total_value_uncertainty": "1.619e-11" + }, "date_created": [ "2015" ], @@ -70587,6 +70706,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.996e+03", + "total_value_uncertainty": "3.068e+00" + }, "date_created": [ "2015" ], @@ -70859,6 +70985,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.278e-02", + "total_value_uncertainty": "7.454e-06" + }, "date_created": [ "2015" ], @@ -71046,6 +71179,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.505e+02", + "total_value_uncertainty": "5.398e-02" + }, "date_created": [ "2015" ], @@ -71247,6 +71387,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.505e+02", + "total_value_uncertainty": "7.711e-02" + }, "date_created": [ "2015" ], @@ -71448,6 +71595,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.015e-04", + "total_value_uncertainty": "2.362e-07" + }, "date_created": [ "2015" ], @@ -71629,6 +71783,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.016e-04", + "total_value_uncertainty": "2.339e-07" + }, "date_created": [ "2015" ], @@ -71816,6 +71977,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.235e+00", + "total_value_uncertainty": "3.291e-03" + }, "date_created": [ "2015" ], @@ -72003,6 +72171,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.895e-05", + "total_value_uncertainty": "1.672e-08" + }, "date_created": [ "2015" ], @@ -72190,6 +72365,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.703e-06", + "total_value_uncertainty": "1.554e-09" + }, "date_created": [ "2015" ], @@ -72385,6 +72567,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.703e-06", + "total_value_uncertainty": "1.559e-09" + }, "date_created": [ "2015" ], @@ -72586,6 +72775,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.708e-07", + "total_value_uncertainty": "1.561e-10" + }, "date_created": [ "2015" ], @@ -72787,6 +72983,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.137e-01", + "total_value_uncertainty": "1.192e-04" + }, "date_created": [ "2015" ], @@ -72974,6 +73177,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.791e-08", + "total_value_uncertainty": "1.621e-11" + }, "date_created": [ "2015" ], @@ -73211,6 +73421,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.791e-08", + "total_value_uncertainty": "1.628e-11" + }, "date_created": [ "2015" ], @@ -73398,6 +73615,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.278e-02", + "total_value_uncertainty": "7.422e-06" + }, "date_created": [ "2015" ], @@ -73585,6 +73809,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.277e-02", + "total_value_uncertainty": "7.435e-06" + }, "date_created": [ "2015" ], @@ -73773,6 +74004,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.505e+02", + "total_value_uncertainty": "5.471e-02" + }, "date_created": [ "2015" ], @@ -73989,6 +74227,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.505e+02", + "total_value_uncertainty": "7.709e-02" + }, "date_created": [ "2015" ], @@ -74177,6 +74422,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.021e-04", + "total_value_uncertainty": "2.364e-07" + }, "date_created": [ "2015" ], @@ -74378,6 +74630,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.230e+00", + "total_value_uncertainty": "3.291e-03" + }, "date_created": [ "2015" ], @@ -74565,6 +74824,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.230e+00", + "total_value_uncertainty": "3.296e-03" + }, "date_created": [ "2015" ], @@ -74753,6 +75019,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.901e-05", + "total_value_uncertainty": "1.677e-08" + }, "date_created": [ "2015" ], @@ -74940,6 +75213,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.895e-05", + "total_value_uncertainty": "1.675e-08" + }, "date_created": [ "2015" ], @@ -75128,6 +75408,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.699e-06", + "total_value_uncertainty": "1.553e-09" + }, "date_created": [ "2015" ], @@ -75343,6 +75630,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.707e-07", + "total_value_uncertainty": "1.554e-10" + }, "date_created": [ "2015" ], @@ -75566,6 +75860,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.707e-07", + "total_value_uncertainty": "1.555e-10" + }, "date_created": [ "2015" ], @@ -75767,6 +76068,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.135e-01", + "total_value_uncertainty": "1.190e-04" + }, "date_created": [ "2015" ], @@ -75954,6 +76262,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.139e-01", + "total_value_uncertainty": "1.204e-04" + }, "date_created": [ "2015" ], @@ -76142,6 +76457,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.787e-08", + "total_value_uncertainty": "1.618e-11" + }, "date_created": [ "2015" ], @@ -76351,6 +76673,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.787e-08", + "total_value_uncertainty": "1.625e-11" + }, "date_created": [ "2015" ], @@ -76552,6 +76881,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.620e+00", + "total_value_uncertainty": "2.717e-03" + }, "date_created": [ "2015" ], @@ -76739,6 +77075,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.147e-01", + "total_value_uncertainty": "2.206e-04" + }, "date_created": [ "2015" ], @@ -76955,6 +77298,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.029e-01", + "total_value_uncertainty": "6.833e-05" + }, "date_created": [ "2015" ], @@ -77185,6 +77535,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.448e-01", + "total_value_uncertainty": "1.300e-05" + }, "date_created": [ "2015" ], @@ -77401,6 +77758,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.662e+00", + "total_value_uncertainty": "1.469e-04" + }, "date_created": [ "2015" ], @@ -77617,6 +77981,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.422e+00", + "total_value_uncertainty": "1.458e-04" + }, "date_created": [ "2015" ], @@ -77833,6 +78204,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.063e-02", + "total_value_uncertainty": "3.334e-05" + }, "date_created": [ "2015" ], @@ -78041,6 +78419,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.675e-01", + "total_value_uncertainty": "6.729e-06" + }, "date_created": [ "2015" ], @@ -78263,6 +78648,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.122e-01", + "total_value_uncertainty": "7.118e-06" + }, "date_created": [ "2015" ], @@ -78499,6 +78891,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.572e+01", + "total_value_uncertainty": "6.801e-02" + }, "date_created": [ "2015" ], @@ -78730,6 +79129,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.048e+01", + "total_value_uncertainty": "8.367e-03" + }, "date_created": [ "2015" ], @@ -78952,6 +79358,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.048e+01", + "total_value_uncertainty": "8.367e-03" + }, "date_created": [ "2015" ], @@ -79174,6 +79587,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.048e+01", + "total_value_uncertainty": "8.366e-03" + }, "date_created": [ "2015" ], @@ -79396,6 +79816,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.048e+01", + "total_value_uncertainty": "8.367e-03" + }, "date_created": [ "2015" ], @@ -79618,6 +80045,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.048e+01", + "total_value_uncertainty": "8.367e-03" + }, "date_created": [ "2015" ], @@ -79826,6 +80260,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.048e+01", + "total_value_uncertainty": "8.367e-03" + }, "date_created": [ "2015" ], @@ -80034,6 +80475,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.048e+01", + "total_value_uncertainty": "8.367e-03" + }, "date_created": [ "2015" ], @@ -80242,6 +80690,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.048e+01", + "total_value_uncertainty": "8.367e-03" + }, "date_created": [ "2015" ], @@ -80450,6 +80905,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.520e+01", + "total_value_uncertainty": "3.608e-02" + }, "date_created": [ "2015" ], @@ -80658,6 +81120,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.619e+01", + "total_value_uncertainty": "7.161e-02" + }, "date_created": [ "2015" ], @@ -80903,6 +81372,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.353e+01", + "total_value_uncertainty": "3.475e-02" + }, "date_created": [ "2015" ], @@ -81167,6 +81643,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.353e+01", + "total_value_uncertainty": "3.475e-02" + }, "date_created": [ "2015" ], @@ -81375,6 +81858,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.310e+01", + "total_value_uncertainty": "6.872e-04" + }, "date_created": [ "2015" ], @@ -81583,6 +82073,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "6.430e+01", + "total_value_uncertainty": "2.825e-02" + }, "date_created": [ "2015" ], @@ -81770,6 +82267,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.086e-01", + "total_value_uncertainty": "2.024e-04" + }, "date_created": [ "2015" ], @@ -82000,6 +82504,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.651e-01", + "total_value_uncertainty": "1.724e-04" + }, "date_created": [ "2015" ], @@ -82216,6 +82727,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.123e-02", + "total_value_uncertainty": "4.251e-05" + }, "date_created": [ "2015" ], @@ -82446,6 +82964,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.485e-02", + "total_value_uncertainty": "1.559e-06" + }, "date_created": [ "2015" ], @@ -82662,6 +83187,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.894e-01", + "total_value_uncertainty": "2.676e-05" + }, "date_created": [ "2015" ], @@ -82878,6 +83410,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.587e-01", + "total_value_uncertainty": "2.840e-05" + }, "date_created": [ "2015" ], @@ -83094,6 +83633,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.702e+00", + "total_value_uncertainty": "6.493e-03" + }, "date_created": [ "2015" ], @@ -83324,6 +83870,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.074e+01", + "total_value_uncertainty": "1.468e-02" + }, "date_created": [ "2015" ], @@ -83611,6 +84164,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "3.067e+00", + "total_value_uncertainty": "4.824e-03" + }, "date_created": [ "2015" ], @@ -83828,6 +84388,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.599e+00", + "total_value_uncertainty": "6.741e-03" + }, "date_created": [ "2015" ], @@ -84115,6 +84682,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "4.695e+00", + "total_value_uncertainty": "5.635e-03" + }, "date_created": [ "2015" ], @@ -84385,6 +84959,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "0.000e+00", + "total_value_uncertainty": "0.000e+00" + }, "date_created": [ "2015" ], @@ -84593,6 +85174,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.822e+00", + "total_value_uncertainty": "7.463e-05" + }, "date_created": [ "2015" ], @@ -84801,6 +85389,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.343e+01", + "total_value_uncertainty": "1.049e-02" + }, "date_created": [ "2015" ], @@ -85002,6 +85597,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "5.565e-02", + "total_value_uncertainty": "5.500e-05" + }, "date_created": [ "2015" ], diff --git a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_14.json b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_14.json index 107cbceea3..179168d70c 100644 --- a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_14.json +++ b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2015-part_14.json @@ -6230,6 +6230,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.240e+02", + "total_value_uncertainty": "1.754e-01" + }, "date_created": [ "2015" ], @@ -22163,6 +22170,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.345e+01", + "total_value_uncertainty": "2.805e-02" + }, "date_created": [ "2015" ], @@ -22379,6 +22393,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.350e+01", + "total_value_uncertainty": "3.877e-02" + }, "date_created": [ "2015" ], @@ -22595,6 +22616,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.570e-02", + "total_value_uncertainty": "2.454e-04" + }, "date_created": [ "2015" ], @@ -22867,6 +22895,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "9.543e-02", + "total_value_uncertainty": "1.514e-04" + }, "date_created": [ "2015" ], @@ -23083,6 +23118,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.582e+01", + "total_value_uncertainty": "7.822e-03" + }, "date_created": [ "2015" ], @@ -23355,6 +23397,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.588e+01", + "total_value_uncertainty": "1.094e-02" + }, "date_created": [ "2015" ], @@ -23571,6 +23620,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "2.304e-03", + "total_value_uncertainty": "3.471e-06" + }, "date_created": [ "2015" ], @@ -23801,6 +23857,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + 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"total_value_uncertainty": "5.152e-03" + }, "date_created": [ "2015" ], @@ -24945,6 +25190,13 @@ "energy": "13TeV", "type": "pp" }, + "cross_section": { + "filter_efficiency": "1.000e+00", + "matching_efficiency": "", + "neg_weight_fraction": "", + "total_value": "1.398e-02", + "total_value_uncertainty": "1.496e-05" + }, "date_created": [ "2015" ], diff --git a/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2016-pileup.json b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2016-pileup.json new file mode 100644 index 0000000000..87abeac4c1 --- /dev/null +++ b/cernopendata/modules/fixtures/data/records/cms-simulated-datasets-2016-pileup.json @@ -0,0 +1,2488 @@ +[ + { + "abstract": { + "description": "

Simulated dataset Neutrino_E-10_gun in PREMIX format for 2016 collision data. Events are sampled from this dataset and added to simulated data to make them comparable with the 2016 collision data, see the guide to pile-up simulation.

See the description of the simulated dataset names in: About CMS simulated dataset names.

This is a sample (10%) of the original dataset.

" + }, + "accelerator": "CERN-LHC", + "categories": { + "primary": "Pileup", + "source": "CMS Collaboration" + }, + "collaboration": { + "name": "CMS Collaboration", + "recid": "" + }, + "collections": [ + "CMS-Simulated-Datasets" + ], + "collision_information": { + "energy": "13TeV", + "type": "pp" + }, + "date_created": [ + "2016" + ], + "date_published": "2024", + "date_reprocessed": "2020", + "distribution": { + "formats": [ + "premix", + "root" + ], + "number_events": 27646400, + "number_files": 17279, + "size": 55600743325296 + }, + "doi": "10.7483/OPENDATA.CMS.VWUA.G7SB", + "experiment": [ + "CMS" + ], + "files": [ + { + "checksum": "adler32:c43db880", + "description": "Neutrino_E-10_gunPREMIX dataset file index (1 of 166) for access to data via CMS virtual machine", + "size": 61373, + "type": "index.json", + "uri": 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These data were generated in several steps (see also CMS Monte Carlo production overview):

", + "steps": [ + { + "configuration_files": [ + { + "script": "#!/bin/bash\n\n# GEN Script begin\nrm -f request_fragment_check.py\nwget -q https://raw.githubusercontent.com/cms-sw/genproductions/master/bin/utils/request_fragment_check.py\nchmod +x request_fragment_check.py\n./request_fragment_check.py --bypass_status --prepid PPD-RunIISummer20UL16GEN-00001\nGEN_ERR=$?\nif [ $GEN_ERR -ne 0 ]; then\n echo \"GEN Checking Script returned exit code $GEN_ERR which means there are $GEN_ERR errors\"\n echo \"Validation WILL NOT RUN\"\n echo \"Please correct errors in the request and run validation again\"\n exit $GEN_ERR\nfi\necho \"Running VALIDATION. GEN Request Checking Script returned no errors\"\n# GEN Script end\n\n# Download fragment from McM\ncurl -s -k https://cms-pdmv-prod.web.cern.ch/mcm/public/restapi/requests/get_fragment/PPD-RunIISummer20UL16GEN-00001 --retry 3 --create-dirs -o Configuration/GenProduction/python/PPD-RunIISummer20UL16GEN-00001-fragment.py\n[ -s Configuration/GenProduction/python/PPD-RunIISummer20UL16GEN-00001-fragment.py ] || exit $?;\n\n# Check if fragment contais gridpack path ant that it is in cvmfs\nif grep -q \"gridpacks\" Configuration/GenProduction/python/PPD-RunIISummer20UL16GEN-00001-fragment.py; then\n if ! grep -q \"/cvmfs/cms.cern.ch/phys_generator/gridpacks\" Configuration/GenProduction/python/PPD-RunIISummer20UL16GEN-00001-fragment.py; then\n echo \"Gridpack inside fragment is not in cvmfs.\"\n exit -1\n fi\nfi\n\n# Dump actual test code to a PPD-RunIISummer20UL16GEN-00001_test.sh file that can be run in Singularity\ncat <<'EndOfTestFile' > PPD-RunIISummer20UL16GEN-00001_test.sh\n#!/bin/bash\n\nexport SCRAM_ARCH=slc7_amd64_gcc700\n\nsource /cvmfs/cms.cern.ch/cmsset_default.sh\nif [ -r CMSSW_10_6_17_patch1/src ] ; then\n echo release CMSSW_10_6_17_patch1 already exists\nelse\n scram p CMSSW CMSSW_10_6_17_patch1\nfi\ncd CMSSW_10_6_17_patch1/src\neval `scram runtime -sh`\n\nmv ../../Configuration .\nscram b\ncd ../..\n\n# Maximum validation duration: 28800s\n# Margin for validation duration: 30%\n# Validation duration with margin: 28800 * (1 - 0.30) = 20160s\n# Time per event for each sequence: 0.0474s\n# Threads for each sequence: 1\n# Time per event for single thread for each sequence: 1 * 0.0474s = 0.0474s\n# Which adds up to 0.0474s per event\n# Single core events that fit in validation duration: 20160s / 0.0474s = 425652\n# Produced events limit in McM is 10000\n# According to 1.0000 efficiency, validation should run 10000 / 1.0000 = 10000 events to reach the limit of 10000\n# Take the minimum of 425652 and 10000, but more than 0 -> 10000\n# It is estimated that this validation will produce: 10000 * 1.0000 = 10000 events\nEVENTS=10000\n\n\n# cmsDriver command\ncmsDriver.py Configuration/GenProduction/python/PPD-RunIISummer20UL16GEN-00001-fragment.py --python_filename PPD-RunIISummer20UL16GEN-00001_1_cfg.py --eventcontent RAWSIM --customise Configuration/DataProcessing/Utils.addMonitoring --datatier GEN --fileout file:PPD-RunIISummer20UL16GEN-00001.root --conditions 106X_mcRun2_asymptotic_v13 --beamspot Realistic25ns13TeV2016Collision --customise_commands process.source.numberEventsInLuminosityBlock=\"cms.untracked.uint32(100)\" --step GEN --geometry DB:Extended --era Run2_2016 --no_exec --mc -n $EVENTS || exit $? ;\n\n# Run generated config\nREPORT_NAME=PPD-RunIISummer20UL16GEN-00001_report.xml\n# Run the cmsRun\ncmsRun -e -j $REPORT_NAME PPD-RunIISummer20UL16GEN-00001_1_cfg.py || exit $? ;\n\n# Parse values from PPD-RunIISummer20UL16GEN-00001_report.xml report\nprocessedEvents=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\nproducedEvents=$(grep -Po \"(?<=)(\\d*)(?=)\" $REPORT_NAME | tail -n 1)\nthreads=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\npeakValueRss=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\npeakValueVsize=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalSize=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalSizeAlt=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalJobTime=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalJobCPU=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\neventThroughput=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\navgEventTime=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\nif [ -z \"$threads\" ]; then\n echo \"Could not find NumberOfThreads in report, defaulting to 1\"\n threads=1\nfi\nif [ -z \"$eventThroughput\" ]; then\n eventThroughput=$(bc -l <<< \"scale=4; 1 / ($avgEventTime / $threads)\")\nfi\nif [ -z \"$totalSize\" ]; then\n totalSize=$totalSizeAlt\nfi\nif [ -z \"$processedEvents\" ]; then\n processedEvents=$EVENTS\nfi\necho \"Validation report of PPD-RunIISummer20UL16GEN-00001 sequence 1/1\"\necho \"Processed events: $processedEvents\"\necho \"Produced events: $producedEvents\"\necho \"Threads: $threads\"\necho \"Peak value RSS: $peakValueRss MB\"\necho \"Peak value Vsize: $peakValueVsize MB\"\necho \"Total size: $totalSize MB\"\necho \"Total job time: $totalJobTime s\"\necho \"Total CPU time: $totalJobCPU s\"\necho \"Event throughput: $eventThroughput\"\necho \"CPU efficiency: \"$(bc -l <<< \"scale=2; ($totalJobCPU * 100) / ($threads * $totalJobTime)\")\" %\"\necho \"Size per event: \"$(bc -l <<< \"scale=4; ($totalSize * 1024 / $producedEvents)\")\" kB\"\necho \"Time per event: \"$(bc -l <<< \"scale=4; (1 / $eventThroughput)\")\" s\"\necho \"Filter efficiency percent: \"$(bc -l <<< \"scale=8; ($producedEvents * 100) / $processedEvents\")\" %\"\necho \"Filter efficiency fraction: \"$(bc -l <<< \"scale=10; ($producedEvents) / $processedEvents\")\n\n# End of PPD-RunIISummer20UL16GEN-00001_test.sh file\nEndOfTestFile\n\n# Make file executable\nchmod +x PPD-RunIISummer20UL16GEN-00001_test.sh\n\nif [ -e \"/cvmfs/unpacked.cern.ch/registry.hub.docker.com/cmssw/el7:amd64\" ]; then\n CONTAINER_NAME=\"el7:amd64\"\nelif [ -e \"/cvmfs/unpacked.cern.ch/registry.hub.docker.com/cmssw/el7:x86_64\" ]; then\n CONTAINER_NAME=\"el7:x86_64\"\nelse\n echo \"Could not find amd64 or x86_64 for el7\"\n exit 1\nfi\n# Run in singularity container\n# Mount afs, eos, cvmfs\n# Mount /etc/grid-security for xrootd\nexport SINGULARITY_CACHEDIR=\"/tmp/$(whoami)/singularity\"\nsingularity run -B /afs -B /eos -B /cvmfs -B /etc/grid-security -B /etc/pki/ca-trust --home $PWD:$PWD /cvmfs/unpacked.cern.ch/registry.hub.docker.com/cmssw/$CONTAINER_NAME $(echo $(pwd)/PPD-RunIISummer20UL16GEN-00001_test.sh)\n", + "title": "Production script" + }, + { + "script": "import FWCore.ParameterSet.Config as cms\n\nfrom Configuration.Generator.Pythia8CommonSettings_cfi import *\nfrom Configuration.Generator.MCTunes2017.PythiaCP5Settings_cfi import *\n\ngenerator = cms.EDFilter(\"Pythia8GeneratorFilter\",\n maxEventsToPrint = cms.untracked.int32(1),\n pythiaPylistVerbosity = cms.untracked.int32(1),\n filterEfficiency = cms.untracked.double(1.0),\n pythiaHepMCVerbosity = cms.untracked.bool(False),\n comEnergy = cms.double(13000.),\n PythiaParameters = cms.PSet(\n pythia8CommonSettingsBlock,\n pythia8CP5SettingsBlock,\n processParameters = cms.vstring(\n 'SoftQCD:inelastic = on',\n ),\n parameterSets = cms.vstring('pythia8CommonSettings',\n 'pythia8CP5Settings',\n 'processParameters',\n )\n )\n)", + "title": "Generator parameters", + "url": "https://cms-pdmv-prod.web.cern.ch/mcm/public/restapi/requests/get_fragment/PPD-RunIISummer20UL16GEN-00001" + }, + { + "cms_confdb_id": "d762e23304ef73cf0335517bd6e0563c", + "process": "GEN", + "title": "Configuration file" + } + ], + "generators": [ + "Pythia8" + ], + "global_tag": "106X_mcRun2_asymptotic_v13", + "output_dataset": "/MinBias_TuneCP5_13TeV-pythia8/RunIISummer20UL16GEN-106X_mcRun2_asymptotic_v13-v2/GEN", + "release": "CMSSW_10_6_17_patch1", + "type": "GEN" + }, + { + "configuration_files": [ + { + "script": "#!/bin/bash\n\n\n# Dump actual test code to a PPD-RunIISummer20UL16SIM-00001_test.sh file that can be run in Singularity\ncat <<'EndOfTestFile' > PPD-RunIISummer20UL16SIM-00001_test.sh\n#!/bin/bash\n\nexport SCRAM_ARCH=slc7_amd64_gcc700\n\nsource /cvmfs/cms.cern.ch/cmsset_default.sh\nif [ -r CMSSW_10_6_17_patch1/src ] ; then\n echo release CMSSW_10_6_17_patch1 already exists\nelse\n scram p CMSSW CMSSW_10_6_17_patch1\nfi\ncd CMSSW_10_6_17_patch1/src\neval `scram runtime -sh`\n\nmv ../../Configuration .\nscram b\ncd ../..\n\n# Maximum validation duration: 28800s\n# Margin for validation duration: 30%\n# Validation duration with margin: 28800 * (1 - 0.30) = 20160s\n# Time per event for each sequence: 13.3371s\n# Threads for each sequence: 8\n# Time per event for single thread for each sequence: 8 * 13.3371s = 106.6968s\n# Which adds up to 106.6968s per event\n# Single core events that fit in validation duration: 20160s / 106.6968s = 188\n# Produced events limit in McM is 10000\n# According to 1.0000 efficiency, validation should run 10000 / 1.0000 = 10000 events to reach the limit of 10000\n# Take the minimum of 188 and 10000, but more than 0 -> 188\n# It is estimated that this validation will produce: 188 * 1.0000 = 188 events\nEVENTS=188\n\n\n# cmsDriver command\ncmsDriver.py --python_filename PPD-RunIISummer20UL16SIM-00001_1_cfg.py --eventcontent RAWSIM --customise Configuration/DataProcessing/Utils.addMonitoring --datatier GEN-SIM --fileout file:PPD-RunIISummer20UL16SIM-00001.root --conditions 106X_mcRun2_asymptotic_v13 --beamspot Realistic25ns13TeV2016Collision --step SIM --geometry DB:Extended --filein \"dbs:/MinBias_TuneCP5_13TeV-pythia8/RunIISummer20UL16GEN-106X_mcRun2_asymptotic_v13-v2/GEN\" --era Run2_2016 --runUnscheduled --no_exec --mc -n $EVENTS || exit $? ;\n\n# Run generated config\nREPORT_NAME=PPD-RunIISummer20UL16SIM-00001_report.xml\n# Run the cmsRun\ncmsRun -e -j $REPORT_NAME PPD-RunIISummer20UL16SIM-00001_1_cfg.py || exit $? ;\n\n# Parse values from PPD-RunIISummer20UL16SIM-00001_report.xml report\nprocessedEvents=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\nproducedEvents=$(grep -Po \"(?<=)(\\d*)(?=)\" $REPORT_NAME | tail -n 1)\nthreads=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\npeakValueRss=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\npeakValueVsize=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalSize=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalSizeAlt=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalJobTime=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalJobCPU=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\neventThroughput=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\navgEventTime=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\nif [ -z \"$threads\" ]; then\n echo \"Could not find NumberOfThreads in report, defaulting to 1\"\n threads=1\nfi\nif [ -z \"$eventThroughput\" ]; then\n eventThroughput=$(bc -l <<< \"scale=4; 1 / ($avgEventTime / $threads)\")\nfi\nif [ -z \"$totalSize\" ]; then\n totalSize=$totalSizeAlt\nfi\nif [ -z \"$processedEvents\" ]; then\n processedEvents=$EVENTS\nfi\necho \"Validation report of PPD-RunIISummer20UL16SIM-00001 sequence 1/1\"\necho \"Processed events: $processedEvents\"\necho \"Produced events: $producedEvents\"\necho \"Threads: $threads\"\necho \"Peak value RSS: $peakValueRss MB\"\necho \"Peak value Vsize: $peakValueVsize MB\"\necho \"Total size: $totalSize MB\"\necho \"Total job time: $totalJobTime s\"\necho \"Total CPU time: $totalJobCPU s\"\necho \"Event throughput: $eventThroughput\"\necho \"CPU efficiency: \"$(bc -l <<< \"scale=2; ($totalJobCPU * 100) / ($threads * $totalJobTime)\")\" %\"\necho \"Size per event: \"$(bc -l <<< \"scale=4; ($totalSize * 1024 / $producedEvents)\")\" kB\"\necho \"Time per event: \"$(bc -l <<< \"scale=4; (1 / $eventThroughput)\")\" s\"\necho \"Filter efficiency percent: \"$(bc -l <<< \"scale=8; ($producedEvents * 100) / $processedEvents\")\" %\"\necho \"Filter efficiency fraction: \"$(bc -l <<< \"scale=10; ($producedEvents) / $processedEvents\")\n\n# End of PPD-RunIISummer20UL16SIM-00001_test.sh file\nEndOfTestFile\n\n# Make file executable\nchmod +x PPD-RunIISummer20UL16SIM-00001_test.sh\n\nif [ -e \"/cvmfs/unpacked.cern.ch/registry.hub.docker.com/cmssw/el7:amd64\" ]; then\n CONTAINER_NAME=\"el7:amd64\"\nelif [ -e \"/cvmfs/unpacked.cern.ch/registry.hub.docker.com/cmssw/el7:x86_64\" ]; then\n CONTAINER_NAME=\"el7:x86_64\"\nelse\n echo \"Could not find amd64 or x86_64 for el7\"\n exit 1\nfi\n# Run in singularity container\n# Mount afs, eos, cvmfs\n# Mount /etc/grid-security for xrootd\nexport SINGULARITY_CACHEDIR=\"/tmp/$(whoami)/singularity\"\nsingularity run -B /afs -B /eos -B /cvmfs -B /etc/grid-security -B /etc/pki/ca-trust --home $PWD:$PWD /cvmfs/unpacked.cern.ch/registry.hub.docker.com/cmssw/$CONTAINER_NAME $(echo $(pwd)/PPD-RunIISummer20UL16SIM-00001_test.sh)\n", + "title": "Production script" + }, + { + "cms_confdb_id": "d762e23304ef73cf0335517bd6e08158", + "process": "SIM", + "title": "Configuration file" + } + ], + "global_tag": "106X_mcRun2_asymptotic_v13", + "output_dataset": "/MinBias_TuneCP5_13TeV-pythia8/RunIISummer20UL16SIM-106X_mcRun2_asymptotic_v13-v2/GEN-SIM", + "release": "CMSSW_10_6_17_patch1", + "type": "SIM" + }, + { + "configuration_files": [ + { + "script": "#!/bin/bash\n\n# GEN Script begin\nrm -f request_fragment_check.py\nwget -q https://raw.githubusercontent.com/cms-sw/genproductions/master/bin/utils/request_fragment_check.py\nchmod +x request_fragment_check.py\n./request_fragment_check.py --bypass_status --prepid PPD-RunIISummer20ULPrePremix-00003\nGEN_ERR=$?\nif [ $GEN_ERR -ne 0 ]; then\n echo \"GEN Checking Script returned exit code $GEN_ERR which means there are $GEN_ERR errors\"\n echo \"Validation WILL NOT RUN\"\n echo \"Please correct errors in the request and run validation again\"\n exit $GEN_ERR\nfi\necho \"Running VALIDATION. GEN Request Checking Script returned no errors\"\n# GEN Script end\n\n# Download fragment from McM\ncurl -s -k https://cms-pdmv-prod.web.cern.ch/mcm/public/restapi/requests/get_fragment/PPD-RunIISummer20ULPrePremix-00003 --retry 3 --create-dirs -o Configuration/GenProduction/python/PPD-RunIISummer20ULPrePremix-00003-fragment.py\n[ -s Configuration/GenProduction/python/PPD-RunIISummer20ULPrePremix-00003-fragment.py ] || exit $?;\n\n# Check if fragment contais gridpack path ant that it is in cvmfs\nif grep -q \"gridpacks\" Configuration/GenProduction/python/PPD-RunIISummer20ULPrePremix-00003-fragment.py; then\n if ! grep -q \"/cvmfs/cms.cern.ch/phys_generator/gridpacks\" Configuration/GenProduction/python/PPD-RunIISummer20ULPrePremix-00003-fragment.py; then\n echo \"Gridpack inside fragment is not in cvmfs.\"\n exit -1\n fi\nfi\n\n# Dump actual test code to a PPD-RunIISummer20ULPrePremix-00003_test.sh file that can be run in Singularity\ncat <<'EndOfTestFile' > PPD-RunIISummer20ULPrePremix-00003_test.sh\n#!/bin/bash\n\nexport SCRAM_ARCH=slc7_amd64_gcc700\n\nsource /cvmfs/cms.cern.ch/cmsset_default.sh\nif [ -r CMSSW_10_6_17_patch1/src ] ; then\n echo release CMSSW_10_6_17_patch1 already exists\nelse\n scram p CMSSW CMSSW_10_6_17_patch1\nfi\ncd CMSSW_10_6_17_patch1/src\neval `scram runtime -sh`\n\nmv ../../Configuration .\nscram b\ncd ../..\n\n# Maximum validation duration: 28800s\n# Margin for validation duration: 30%\n# Validation duration with margin: 28800 * (1 - 0.30) = 20160s\n# Time per event for each sequence: 17.7118s\n# Threads for each sequence: 1\n# Time per event for single thread for each sequence: 1 * 17.7118s = 17.7118s\n# Which adds up to 17.7118s per event\n# Single core events that fit in validation duration: 20160s / 17.7118s = 1138\n# Produced events limit in McM is 10000\n# According to 1.0000 efficiency, validation should run 10000 / 1.0000 = 10000 events to reach the limit of 10000\n# Take the minimum of 1138 and 10000, but more than 0 -> 1138\n# It is estimated that this validation will produce: 1138 * 1.0000 = 1138 events\nEVENTS=1138\n\n\n# cmsDriver command\ncmsDriver.py Configuration/GenProduction/python/PPD-RunIISummer20ULPrePremix-00003-fragment.py --python_filename PPD-RunIISummer20ULPrePremix-00003_1_cfg.py --eventcontent PREMIX --pileup 2016_25ns_UltraLegacy_PoissonOOTPU --customise Configuration/DataProcessing/Utils.addMonitoring --datatier PREMIX --fileout file:PPD-RunIISummer20ULPrePremix-00003.root --pileup_input \"dbs:/MinBias_TuneCP5_13TeV-pythia8/RunIISummer20UL16SIM-106X_mcRun2_asymptotic_v13-v2/GEN-SIM\" --conditions 106X_mcRun2_asymptotic_v13 --customise_commands process.source.numberEventsInLuminosityBlock=\"cms.untracked.uint32(100)\" --step GEN,SIM,DIGI --procModifiers premix_stage1 --geometry DB:Extended --era Run2_2016 --no_exec --mc -n $EVENTS || exit $? ;\n\n# Run generated config\nREPORT_NAME=PPD-RunIISummer20ULPrePremix-00003_report.xml\n# Run the cmsRun\ncmsRun -e -j $REPORT_NAME PPD-RunIISummer20ULPrePremix-00003_1_cfg.py || exit $? ;\n\n# Parse values from PPD-RunIISummer20ULPrePremix-00003_report.xml report\nprocessedEvents=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\nproducedEvents=$(grep -Po \"(?<=)(\\d*)(?=)\" $REPORT_NAME | tail -n 1)\nthreads=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\npeakValueRss=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\npeakValueVsize=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalSize=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalSizeAlt=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalJobTime=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\ntotalJobCPU=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\neventThroughput=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\navgEventTime=$(grep -Po \"(?<=)\" $REPORT_NAME | tail -n 1)\nif [ -z \"$threads\" ]; then\n echo \"Could not find NumberOfThreads in report, defaulting to 1\"\n threads=1\nfi\nif [ -z \"$eventThroughput\" ]; then\n eventThroughput=$(bc -l <<< \"scale=4; 1 / ($avgEventTime / $threads)\")\nfi\nif [ -z \"$totalSize\" ]; then\n totalSize=$totalSizeAlt\nfi\nif [ -z \"$processedEvents\" ]; then\n processedEvents=$EVENTS\nfi\necho \"Validation report of PPD-RunIISummer20ULPrePremix-00003 sequence 1/1\"\necho \"Processed events: $processedEvents\"\necho \"Produced events: $producedEvents\"\necho \"Threads: $threads\"\necho \"Peak value RSS: $peakValueRss MB\"\necho \"Peak value Vsize: $peakValueVsize MB\"\necho \"Total size: $totalSize MB\"\necho \"Total job time: $totalJobTime s\"\necho \"Total CPU time: $totalJobCPU s\"\necho \"Event throughput: $eventThroughput\"\necho \"CPU efficiency: \"$(bc -l <<< \"scale=2; ($totalJobCPU * 100) / ($threads * $totalJobTime)\")\" %\"\necho \"Size per event: \"$(bc -l <<< \"scale=4; ($totalSize * 1024 / $producedEvents)\")\" kB\"\necho \"Time per event: \"$(bc -l <<< \"scale=4; (1 / $eventThroughput)\")\" s\"\necho \"Filter efficiency percent: \"$(bc -l <<< \"scale=8; ($producedEvents * 100) / $processedEvents\")\" %\"\necho \"Filter efficiency fraction: \"$(bc -l <<< \"scale=10; ($producedEvents) / $processedEvents\")\n\n# End of PPD-RunIISummer20ULPrePremix-00003_test.sh file\nEndOfTestFile\n\n# Make file executable\nchmod +x PPD-RunIISummer20ULPrePremix-00003_test.sh\n\nif [ -e \"/cvmfs/unpacked.cern.ch/registry.hub.docker.com/cmssw/el7:amd64\" ]; then\n CONTAINER_NAME=\"el7:amd64\"\nelif [ -e \"/cvmfs/unpacked.cern.ch/registry.hub.docker.com/cmssw/el7:x86_64\" ]; then\n CONTAINER_NAME=\"el7:x86_64\"\nelse\n echo \"Could not find amd64 or x86_64 for el7\"\n exit 1\nfi\n# Run in singularity container\n# Mount afs, eos, cvmfs\n# Mount /etc/grid-security for xrootd\nexport SINGULARITY_CACHEDIR=\"/tmp/$(whoami)/singularity\"\nsingularity run -B /afs -B /eos -B /cvmfs -B /etc/grid-security -B /etc/pki/ca-trust --home $PWD:$PWD /cvmfs/unpacked.cern.ch/registry.hub.docker.com/cmssw/$CONTAINER_NAME $(echo $(pwd)/PPD-RunIISummer20ULPrePremix-00003_test.sh)\n", + "title": "Production script" + }, + { + "cms_confdb_id": "bd6fc1859c555ba6f366001d9c1c61e5", + "process": "DIGI", + "title": "Configuration file" + } + ], + "generators": [ + "Pythia8" + ], + "global_tag": "106X_mcRun2_asymptotic_v13", + "output_dataset": "/Neutrino_E-10_gun/RunIISummer20ULPrePremix-UL16_106X_mcRun2_asymptotic_v13-v1/PREMIX", + "release": "CMSSW_10_6_17_patch1", + "type": "DIGI" + } + ] + }, + "pileup": { + "description": "

To make these simulated data comparable with the collision data, pile-up events from the dataset /MinBias_TuneCP5_13TeV-pythia8/RunIISummer20UL16SIM-106X_mcRun2_asymptotic_v13-v2/GEN-SIM are added to the simulated event in the DIGI step.

" + }, + "publisher": "CERN Open Data Portal", + "recid": "30595", + "run_period": [ + "Run2016G", + "Run2016H" + ], + "system_details": { + "container_images": [ + { + "name": "docker.io/cmsopendata/cmssw_10_6_30-slc7_amd64_gcc700:latest", + "registry": "dockerhub" + }, + { + "name": "gitlab-registry.cern.ch/cms-cloud/cmssw-docker-opendata/cmssw_10_6_30-slc7_amd64_gcc700:latest", + "registry": "gitlab" + } + ], + "global_tag": "106X_mcRun2_asymptotic_v17", + "release": "CMSSW_10_6_30" + }, + "title": "/Neutrino_E-10_gun/RunIISummer20ULPrePremix-UL16_106X_mcRun2_asymptotic_v13-v1/PREMIX", + "title_additional": "Simulated dataset Neutrino_E-10_gun in PREMIX format for 2016 collision data", + "type": { + "primary": "Dataset", + "secondary": [ + "Simulated" + ] + }, + "usage": { + "description": "These simulated data are not meant to be analysed on their own. The dataset can be used to add pile-up events to newly simulated event samples using CMS experiment software, available through the CMS Open Data container or the CMS Virtual Machine. See the instructions for setting up one of the two alternative environments and getting started in", + "links": [ + { + "description": "Running CMS analysis code using Docker", + "url": "/docs/cms-guide-docker#images" + }, + { + "description": "How to install the CMS Virtual Machine", + "url": "/docs/cms-virtual-machine-cc7" + }, + { + "description": "Getting started with CMS open data", + "url": "/docs/cms-getting-started-miniaod" + } + ] + }, + "validation": { + "description": "The generation and simulation of Monte Carlo data has been validated through general CMS validation procedures." + } + } +] diff --git a/cernopendata/modules/fixtures/data/records/cms-tools-pfnano.json b/cernopendata/modules/fixtures/data/records/cms-tools-pfnano.json index e53f3ef97a..b3c092bf74 100644 --- a/cernopendata/modules/fixtures/data/records/cms-tools-pfnano.json +++ b/cernopendata/modules/fixtures/data/records/cms-tools-pfnano.json @@ -44,7 +44,7 @@ ] }, "usage": { - "description": "

PFNanoProducerTool is a producer package to be used with the CMSSW software. The output files are available for Run2016G collision datasets on this portal and they can be analysed independently.

\n

For any additional production, CMSSW is available in the CMS Open Data environments: in the CMS Docker container and in the CMS VM image.

\n\t\t\t

To download and run the PFNanoProducer code, follow the instructions at https://github.com/cms-opendata-analyses/PFNanoProducerTool.

\n

For more information about physics object access, see the CMS Open Data Guide web site.

\n

The output files from the PFNanoProducer package have the usual NanoAOD content and, in addition, the PF candidate information. The files are produced in the ROOT format and their analysis does not require the use of CMSSW and CMS Open data environments.

" + "description": "

PFNanoProducerTool is a producer package to be used with the CMSSW software. The output files are available for Run2016G collision datasets on this portal and they can be analysed independently.

\n

For any additional production, CMSSW is available in the CMS Open Data environments: in the CMS Docker container and in the CMS VM image.

\n\t\t\t

To download and run the PFNanoProducer code, follow the instructions at https://github.com/cms-opendata-analyses/PFNanoProducerTool.

\n

For more information about physics object access, see the CMS Open Data Guide web site.

\n

The output files from the PFNanoProducer package have the usual NanoAOD content and, in addition, the PF candidate information. The files are produced in the ROOT format and their analysis does not require the use of CMSSW and CMS Open data environments.

" }, "use_with": { "description": "Use this software with any CMS 2016 MiniAOD or MiniAODSIM datasets." diff --git a/cernopendata/modules/fixtures/data/records/cms-tools-vm-image-2016-2018.json b/cernopendata/modules/fixtures/data/records/cms-tools-vm-image-2016-2018.json new file mode 100644 index 0000000000..b4bfd1d659 --- /dev/null +++ b/cernopendata/modules/fixtures/data/records/cms-tools-vm-image-2016-2018.json @@ -0,0 +1,147 @@ +[ + { + "abstract": { + "description": "

This virtual machine image provides CMS computing environment to be used with the CMS MiniAOD open data from 2016 - 2018. The virtual machine is based on CernVM. The image gets the CMS software (CMSSW) from /cvmfs/cms.cern.ch and the jobs running on the VM read the condition data from /cvmfs/cms-opendata-conddb.cern.ch. Access to the data is through XRootD.

It has a 40G virtual hard disk and a 20G cvmfs cache, which is large enough for condition data for full event range for 2016 data (see the CMS guide to the condition database for further details). It has an embedded CERN CentOS (cc7) shell with the architecture compatible with the CMS software version, in which all CMS software specific commands should be executed. Additionally, it has another CERN CentOS 7 (cc7) shell, which can be used in the same session.

For known issues and limitations see

", + "links": [ + { + "title": "CMS CC7 Virtual Machines - Known Issues and Limitations", + "url": "/docs/cms-virtual-machine-cc7#issue" + } + ] + }, + "accelerator": "CERN-LHC", + "collaboration": { + "name": "CMS Collaboration" + }, + "collections": [ + "CMS-Tools" + ], + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "ova" + ], + "number_files": 1, + "size": 20500480 + }, + "experiment": [ + "CMS" + ], + "files": [ + { + "checksum": "adler32:24f015c5", + "size": 20500480, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/environment/1.6.0/CMS-OpenData-1.6.0.ova" + } + ], + "methodology": { + "description": "The contextualisation scripts used for setting up the CMS VM images are available at", + "links": [ + { + "recid": "259" + } + ] + }, + "publisher": "CERN Open Data Portal", + "recid": "258", + "run_period": [ + "Run2016G", + "Run2016H" + ], + "title": "CMS CC7 VM Image, for CMS MiniAOD open data from 2016 - 2018", + "type": { + "primary": "Environment", + "secondary": [ + "VM" + ] + }, + "usage": { + "description": "Please follow the instructions on how to use the CMS Virtual Machine", + "links": [ + { + "description": "CMS CC7 Virtual Machines: How to install", + "url": "/docs/cms-virtual-machine-cc7" + } + ] + } + }, + { + "abstract": { + "description": "

The scripts provided create the CMS virtual machine image based on CernVM, with CERN CentOS 7 (cc7).

" + }, + "accelerator": "CERN-LHC", + "collections": [ + "CMS-Tools" + ], + "date_created": [ + "2016" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "hdd", + "iso", + "sh", + "txt" + ], + "number_files": 5, + "size": 25604650 + }, + "experiment": [ + "CMS" + ], + "files": [ + { + "checksum": "adler32:f13714c4", + "size": 368640, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/environment/1.6.0/CMS-OpenData-1.6.0.context.iso" + }, + { + "checksum": "adler32:180f3ca3", + "size": 196, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/environment/1.6.0/cernvm-script" + }, + { + "checksum": "adler32:175a7154", + "size": 4302, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/environment/1.6.0/cms-user-data.txt" + }, + { + "checksum": "adler32:786f33c7", + "size": 152, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/environment/1.6.0/opendata-desktop-settings" + }, + { + "checksum": "adler32:9c7c8157", + "size": 25231360, + "uri": "root://eospublic.cern.ch//eos/opendata/cms/environment/1.6.0/ucernvm-v4prod.2020.07-1.cernvm.x86_64.hdd" + } + ], + "publisher": "CERN Open Data Portal", + "recid": "259", + "relations": [ + { + "description": "The CERN VM image produced by these scripts can be found here:", + "recid": "258", + "type": "isRelatedTo" + } + ], + "run_period": [ + "Run2016G", + "Run2016H" + ], + "title": "Contextualisation scripts to create the CMS VM Image version 1.6.0", + "type": { + "primary": "Environment", + "secondary": [ + "VM" + ] + }, + "usage": { + "description": "

First, you need to run a normal Micro-CernVM, using your own context so you can login. Copy the attached files to the running VM and then login.

Inside the VM, you need a copy of the latest Micro-CernVM release as a template for the Open Data image. Download the template ucernvm-v4prod.2020.07-1.cernvm.x86_64.hdd from this record, inside the running VM placing it in the same directory as the other files.

Run the script:
./cernvm-script
which will produce some output on the terminal, and then finish.

The result should be a file with the title coming from the -n field in the script, in this case:
CMS-OpenData-1.6.0.ova
which can be copied from the running VM to elsewhere.

" + } + } +] diff --git a/cernopendata/modules/fixtures/data/records/cms-tools-vm-image-Run2011A.json b/cernopendata/modules/fixtures/data/records/cms-tools-vm-image-Run2011A.json index af61d01798..7801fd54e9 100644 --- a/cernopendata/modules/fixtures/data/records/cms-tools-vm-image-Run2011A.json +++ b/cernopendata/modules/fixtures/data/records/cms-tools-vm-image-Run2011A.json @@ -5,7 +5,7 @@ "links": [ { "title": "CMS Virtual Machines - Known Issues and Limitations", - "url": "/VM/CMS/2011#issue" + "url": "/docs/cms-virtual-machine-2015#issue" } ] }, diff --git a/cernopendata/modules/fixtures/data/records/cms-tools-vm-image.json b/cernopendata/modules/fixtures/data/records/cms-tools-vm-image.json index ddc55d8352..fa41eb8726 100644 --- a/cernopendata/modules/fixtures/data/records/cms-tools-vm-image.json +++ b/cernopendata/modules/fixtures/data/records/cms-tools-vm-image.json @@ -5,7 +5,7 @@ "links": [ { "title": "CMS Virtual Machines - Known Issues and Limitations", - "url": "/VM/CMS/2010#issues2010" + "url": "/docs/cms-virtual-machine-2010#issues2010" } ] }, @@ -76,7 +76,7 @@ "links": [ { "description": "CMS Virtual Machines: How to install", - "url": "/VM/CMS/2010" + "url": "/docs/cms-virtual-machine-2010" } ] }, diff --git a/cernopendata/modules/fixtures/data/records/jade-computing-notes.json b/cernopendata/modules/fixtures/data/records/jade-computing-notes.json new file mode 100644 index 0000000000..126c67f433 --- /dev/null +++ b/cernopendata/modules/fixtures/data/records/jade-computing-notes.json @@ -0,0 +1,6073 @@ +[ + { + "abstract": { + "description": "Index" + }, + "accelerator": "DESY-PETRA", + "collaboration": { + "name": "JADE collaboration", + "recid": "26050" + }, + "collections": [ + "JADE-Computing-Notes" + ], + "date_created": [ + "1989" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "pdf" + ], + "number_files": 1, + "size": 137529 + }, + "experiment": [ + "JADE" + ], + "files": [ + { + "checksum": 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"abstract": { + "description": "Changes to dE/dx routines and description of Bank JHQT" + }, + "accelerator": "DESY-PETRA", + "authors": [ + { + "name": "Elsen" + }, + { + "name": "Ambrus" + } + ], + "collaboration": { + "name": "JADE collaboration", + "recid": "26050" + }, + "collections": [ + "JADE-Computing-Notes" + ], + "date_created": [ + "1987" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "pdf" + ], + "number_files": 1, + "size": 82304 + }, + "experiment": [ + "JADE" + ], + "files": [ + { + "checksum": "adler32:4518c8b8", + "size": 82304, + "uri": "root://eospublic.cern.ch//eos/opendata/jade/documentation/notes/96.pdf" + } + ], + "license": { + "attribution": "CC0" + }, + "publisher": "CERN Open Data Portal", + "recid": "26263", + "title": "JADE Computing Note 96", + "type": { + "primary": "Supplementaries", + "secondary": [ + "Computing Note" + ] + } + }, + { + "abstract": { + "description": "dE/dx Monte Carlo" + }, + "accelerator": "DESY-PETRA", + "authors": [ + { + "name": "Elsen" + } + ], + "collaboration": { + "name": "JADE collaboration", + "recid": "26050" + }, + "collections": [ + "JADE-Computing-Notes" + ], + "date_created": [ + "1987" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "pdf" + ], + "number_files": 1, + "size": 293114 + }, + "experiment": [ + "JADE" + ], + "files": [ + { + "checksum": "adler32:a74e4c63", + "size": 293114, + "uri": "root://eospublic.cern.ch//eos/opendata/jade/documentation/notes/97.pdf" + } + ], + "license": { + "attribution": "CC0" + }, + "publisher": "CERN Open Data Portal", + "recid": "26264", + "title": "JADE Computing Note 97", + "type": { + "primary": "Supplementaries", + "secondary": [ + "Computing Note" + ] + } + }, + { + "abstract": { + "description": "Minutes of the JADE software meeting of Dec. 14 1987 at DESY" + }, + "accelerator": "DESY-PETRA", + "authors": [ + { + "name": "Bartel" + } + ], + "collaboration": { + "name": "JADE collaboration", + "recid": "26050" + }, + "collections": [ + "JADE-Computing-Notes" + ], + "date_created": [ + "1988" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "pdf" + ], + "number_files": 1, + "size": 2485521 + }, + "experiment": [ + "JADE" + ], + "files": [ + { + "checksum": "adler32:080e0c4f", + "size": 2485521, + "uri": "root://eospublic.cern.ch//eos/opendata/jade/documentation/notes/98.pdf" + } + ], + "license": { + "attribution": "CC0" + }, + "publisher": "CERN Open Data Portal", + "recid": "26265", + "title": "JADE Computing Note 98", + "type": { + "primary": "Supplementaries", + "secondary": [ + "Computing Note" + ] + } + }, + { + "abstract": { + "description": "A new compact data format: description of bank ZE4V" + }, + "accelerator": "DESY-PETRA", + "authors": [ + { + "name": "Eckerlin" + }, + { + "name": "Zimmer" + } + ], + "collaboration": { + "name": "JADE collaboration", + "recid": "26050" + }, + "collections": [ + "JADE-Computing-Notes" + ], + "date_created": [ + "1988" + ], + "date_published": "2024", + "distribution": { + "formats": [ + "pdf" + ], + "number_files": 1, + "size": 329116 + }, + "experiment": [ + "JADE" + ], + "files": [ + { + "checksum": "adler32:778977ed", + "size": 329116, + "uri": "root://eospublic.cern.ch//eos/opendata/jade/documentation/notes/99.pdf" + } + ], + "license": { + "attribution": "CC0" + }, + "publisher": "CERN Open Data Portal", + "recid": "26266", + "title": "JADE Computing Note 99", + "type": { + "primary": "Supplementaries", + "secondary": [ + "Computing Note" + ] + } + } +] diff --git a/cernopendata/modules/records/serializers/basic_json.py b/cernopendata/modules/records/serializers/basic_json.py index a0a87778d7..8cad443048 100644 --- a/cernopendata/modules/records/serializers/basic_json.py +++ b/cernopendata/modules/records/serializers/basic_json.py @@ -53,7 +53,7 @@ def serialize_search( """Serialize a search result. :param pid_fetcher: Persistent identifier fetcher. - :param search_result: Elasticsearch search result. + :param search_result: OpenSearch search result. :param links: Dictionary of links to add to response. """ total = search_result["hits"]["total"]["value"] diff --git a/cernopendata/modules/theme/assets/semantic-ui/js/records/components/FileTable.js b/cernopendata/modules/theme/assets/semantic-ui/js/records/components/FileTable.js index 388e86421d..5d1dff2727 100644 --- a/cernopendata/modules/theme/assets/semantic-ui/js/records/components/FileTable.js +++ b/cernopendata/modules/theme/assets/semantic-ui/js/records/components/FileTable.js @@ -60,6 +60,7 @@ export default function FileTable({ items }) { }, } : { href: getFileUri(file.key) }; + const label = file.type == 'index.txt' ? 'Download index' : 'Download'; return ( {file.key} @@ -80,7 +81,7 @@ export default function FileTable({ items }) { )} diff --git a/cernopendata/modules/theme/static/docs/cms-pileup-simulation/MC2016_PU.png b/cernopendata/modules/theme/static/docs/cms-pileup-simulation/MC2016_PU.png new file mode 100644 index 0000000000..cb1a232374 Binary files /dev/null and b/cernopendata/modules/theme/static/docs/cms-pileup-simulation/MC2016_PU.png differ diff --git a/cernopendata/modules/theme/static/docs/cms-virtual-machine-cc7/cms_vm_cc7_1.png b/cernopendata/modules/theme/static/docs/cms-virtual-machine-cc7/cms_vm_cc7_1.png new file mode 100644 index 0000000000..d1720820ce Binary files /dev/null and b/cernopendata/modules/theme/static/docs/cms-virtual-machine-cc7/cms_vm_cc7_1.png differ diff --git a/cernopendata/templates/cernopendata_records_ui/records/record_detail.html b/cernopendata/templates/cernopendata_records_ui/records/record_detail.html index 95e569ae00..678fdb0747 100644 --- a/cernopendata/templates/cernopendata_records_ui/records/record_detail.html +++ b/cernopendata/templates/cernopendata_records_ui/records/record_detail.html @@ -103,6 +103,25 @@

Preview

{%include "cernopendata_ispy/ispy_standalone.html"%} {% endif %} + {% if record.cross_section %} +

Cross section

+ {% if record.cross_section.description %} + {{record.cross_section.description | safe}} +
+ {% else %} +

For {{record.collision_information.type }} collisions at {{record.collision_information.energy }}, this sample has a cross section of ({{record.cross_section.total_value }} +/- {{record.cross_section.total_value_uncertainty }}) pb, calculated using the method described in CMS guide for cross sections.

+ {% endif %} + {% if record.cross_section.matching_efficiency %} +

This cross section takes into account a matching efficiency of {{record.cross_section.matching_efficiency }} and a filtering efficiency of {{record.cross_section.filter_efficiency }}, based on generator settings and/or filters.

+ {% else %} +

This cross section takes into account a filtering efficiency of {{record.cross_section.filter_efficiency }}, based on generator settings and/or filters.

+ {% endif %} + {% if record.cross_section.neg_weight_fraction %} +

If this sample was generated at NLO, it has {{record.cross_section.neg_weight_fraction }}% events with negative weights.

+ {% endif %} +

This is a leading-order value, and cross sections evaluated at next-to-leading order (NLO) or next-to-next-to-leading order (NNLO) should be used, if available.

+ {% endif %} + {% if record.use_with %}

Use with

{{record.use_with.description | safe}}

@@ -210,6 +229,15 @@

System details

{% endif %} + {% if record.dataset_semantics_files %} +
+

Dataset semantics

+ + Variable list + +
+ {% endif %} + {% if record.dataset_semantics %}

Dataset semantics

diff --git a/cernopendata/templates/cernopendata_theme/footer.html b/cernopendata/templates/cernopendata_theme/footer.html index f789527a0d..513e43ef9c 100644 --- a/cernopendata/templates/cernopendata_theme/footer.html +++ b/cernopendata/templates/cernopendata_theme/footer.html @@ -96,9 +96,10 @@
-