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Calorimetry_cff.py
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Calorimetry_cff.py
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import FWCore.ParameterSet.Config as cms
# This is used to modify parameters for Run 2 (see bottom of file)
#Global fast calorimetry parameters
from FastSimulation.Calorimetry.HcalResponse_cfi import *
from FastSimulation.Calorimetry.HSParameters_cfi import *
from Geometry.HcalSimData.HFParameters_cff import *
#from FastSimulation.Configuration.CommonInputs_cff import *
from FastSimulation.Calorimetry.ECALResponse_cfi import *
FamosCalorimetryBlock = cms.PSet(
Calorimetry = cms.PSet(
#ECALScaleBlock, # comment out to disable scaling
HSParameterBlock,
HCALResponseBlock,
ECAL = cms.PSet(
# See FastSimulation/CaloRecHitsProducer/python/CaloRecHits_cff.py
Digitizer = cms.untracked.bool(False),
# If set to true the simulation in ECAL would be done 1X0 by 1X0
# this is slow but more adapted to detailed studies.
# Otherwise roughty 5 steps are used.
bFixedLength = cms.bool(False),
# For the core 10% of the spots for
CoreIntervals = cms.vdouble(100.0, 0.1),
# change the radius of the tail of the shower
RTFactor = cms.double(1.0),
# change the radius of the core of the shower
RCFactor = cms.double(1.0),
# For the tail 10% of r<1RM. 100% otherwise
TailIntervals = cms.vdouble(1.0, 0.1, 100.0, 1.0),
FrontLeakageProbability = cms.double(1.0),
GridSize = cms.int32(7),
# change globally the Moliere radius
### changed after tuning - Feb - July - Shilpi Jain
#RadiusFactor = cms.double(1.096),
RadiusFactorEB = cms.double(1.096),
RadiusFactorEE = cms.double(1.25),
### changed after tuning - Feb - July - Shilpi Jain
RadiusPreshowerCorrections = cms.vdouble(0.137, 10.3), # default value for maxshower depth dependence-->works fine
MipsinGeV = cms.vdouble(0.0001421,0.0000812), # increase in mipsinGeV by 75% only in layer1
#SpotFraction < 0 <=> deactivated. In the case, CoreIntervals and
#TailIntervals are used
SpotFraction = cms.double(-1.0),
GapLossProbability = cms.double(0.9),
SimulatePreshower = cms.bool(True)
),
ForwardCalorimeterProperties = cms.PSet(
HadronicCalorimeterProperties= cms.PSet(
HCAL_Sampling = cms.double(0.0035),
# Watch out ! The following two values are defined wrt the electron shower simulation
# There are not directly related to the detector properties
HCAL_PiOverE = cms.double(0.2),
# HCAL_PiOverE = cms.double(0.4)
HCALAeff= cms.double(55.845),
HCALZeff= cms.double(26),
HCALrho= cms.double(7.87),
HCALradiationLengthIncm= cms.double(1.757),
HCALradLenIngcm2= cms.double(13.84),
HCALmoliereRadius= cms.double(1.719),
HCALcriticalEnergy= cms.double(21E-3),
HCALinteractionLength= cms.double(16.77),
HCALetatow=cms.vdouble( 0.000, 0.087, 0.174, 0.261, 0.348, 0.435, 0.522, 0.609, 0.696, 0.783, 0.870, 0.957, 1.044, 1.131, 1.218, 1.305, 1.392, 1.479, 1.566, 1.653, 1.740, 1.830, 1.930, 2.043, 2.172, 2.322, 2.500, 2.650, 2.853, 3.000, 3.139, 3.314, 3.489, 3.664, 3.839, 4.013, 4.191, 4.363, 4.538, 4.716, 4.889, 5.191),
# HCALDepthLam=cms.vdouble( 8.930, 9.001, 9.132, 8.912, 8.104, 8.571, 8.852, 9.230, 9.732, 10.29, 10.95, 11.68, 12.49, 12.57, 12.63, 6.449, 5.806, 8.973, 8.934, 8.823, 8.727, 8.641, 8.565, 8.496, 8.436, 8.383, 8.346, 8.307, 8.298, 8.281, 9.442, 9.437, 9.432, 9.429, 9.432, 9.433, 9.430, 9.437, 9.442, 9.446, 9.435)
HCALDepthLam=cms.vdouble(8.014, 8.078, 8.195, 7.998, 7.273, 7.692, 7.944, 8.283, 8.734, 9.235, 9.827, 10.482, 11.209, 11.281, 11.335, 5.788, 5.211, 8.053, 8.018, 7.918, 7.832, 7.755, 7.687, 7.625, 7.571, 7.523, 7.490, 7.455, 7.447, 7.432, 8.474, 8.469, 8.465, 8.462, 8.465, 8.466, 8.463, 8.469, 8.474, 8.477, 8.467)
),
),
CalorimeterProperties = cms.PSet(
# triplet for each p value: p, k_e(p), k_h(p) ...
RespCorrP = cms.vdouble(1.0, 1.0, 1.0, 1000.0, 1.0, 1.0),
PreshowerLayer2_thickness = cms.double(0.38), # layer2 thickness back to original
ECALEndcap_LightCollection = cms.double(0.023),
PreshowerLayer1_thickness = cms.double(1.65), # increase in thickness of layer 1 by 3%
PreshowerLayer1_mipsPerGeV = cms.double(17.85), # 50% decrease in mipsperGeV
PreshowerLayer2_mipsPerGeV = cms.double(59.5),
ECALBarrel_LightCollection = cms.double(0.03),
HadronicCalorimeterProperties= cms.PSet(
HCAL_Sampling = cms.double(0.0035),
# Watch out ! The following two values are defined wrt the electron shower simulation
# There are not directly related to the detector properties
HCAL_PiOverE = cms.double(0.2),
# HCAL_PiOverE = cms.double(0.4)
HCALAeff= cms.double(63.546),
HCALZeff= cms.double(29.),
HCALrho= cms.double(8.960),
HCALradiationLengthIncm= cms.double(1.43),
HCALradLenIngcm2= cms.double(12.86),
HCALmoliereRadius= cms.double(1.712),
HCALcriticalEnergy= cms.double(18.63E-3),
HCALinteractionLength= cms.double(15.05),
HCALetatow=cms.vdouble( 0.000, 0.087, 0.174, 0.261, 0.348, 0.435, 0.522, 0.609, 0.696, 0.783, 0.870, 0.957, 1.044, 1.131, 1.218, 1.305, 1.392, 1.479, 1.566, 1.653, 1.740, 1.830, 1.930, 2.043, 2.172, 2.322, 2.500, 2.650, 2.853, 3.000, 3.139, 3.314, 3.489, 3.664, 3.839, 4.013, 4.191, 4.363, 4.538, 4.716, 4.889, 5.191),
HCALDepthLam=cms.vdouble( 8.930, 9.001, 9.132, 8.912, 8.104, 8.571, 8.852, 9.230, 9.732, 10.29, 10.95, 11.68, 12.49, 12.57, 12.63, 6.449, 5.806, 8.973, 8.934, 8.823, 8.727, 8.641, 8.565, 8.496, 8.436, 8.383, 8.346, 8.307, 8.298, 8.281, 9.442, 9.437, 9.432, 9.429, 9.432, 9.433, 9.430, 9.437, 9.442, 9.446, 9.435)
),
BarrelCalorimeterProperties = cms.PSet(
#====== Geometrical material properties ========
# Light Collection efficiency
lightColl = cms.double(0.03),
# Light Collection uniformity
lightCollUnif = cms.double(0.003),
# Photostatistics (photons/GeV) in the homegeneous material
photoStatistics = cms.double(50.E3),
# Thickness of the detector in cm
thickness = cms.double(23.0),
#====== Global parameters of the material ========
# Interaction length in cm
interactionLength = cms.double(18.5),
Aeff = cms.double(170.87),
Zeff = cms.double(68.36),
rho = cms.double(8.280),
# Radiation length in g/cm^2
radLenIngcm2 = cms.double(7.37),
# ===== Those parameters might be entered by hand
# or calculated out of the previous ones
# Radiation length in cm. If value set to -1, FastSim uses internally the
# formula radLenIngcm2/rho
radLenIncm = cms.double(0.89),
# Critical energy in GeV. If value set to -1, FastSim uses internally the
# formula (2.66E-3*(x0*Z/A)^1.1): 8.74E-3 for ECAL EndCap
criticalEnergy = cms.double(8.74E-3),
# Moliere Radius in cm.If value set to -1, FastSim uses internally the
# formula : Es/criticalEnergy*X0 with Es=sqrt(4*Pi/alphaEM)*me*c^2=0.0212 GeV
# This value is known to be 2.190 cm for ECAL Endcap, but the formula gives 2.159 cm
moliereRadius = cms.double(2.190),
#====== Parameters for sampling ECAL ========
# Sampling Fraction: Fs = X0eff/(da+dp) where X0eff is the average X0
# of the active and passive media and da/dp their thicknesses
Fs = cms.double(0.0),
# e/mip for the calorimeter. May be estimated by 1./(1+0.007*(Zp-Za))
ehat = cms.double(0.0),
# a rough estimate of ECAL resolution sigma/E = resE/sqrt(E)
# it is used to generate Nspots in radial profiles.
resE = cms.double(1.),
# the width in cm of the active layer
da = cms.double(0.2),
# the width in cm of the passive layer
dp = cms.double(0.8),
# Is a homogenious detector?
bHom = cms.bool(True),
# Activate the LogDebug
debug = cms.bool(False)
),
EndcapCalorimeterProperties = cms.PSet(
#====== Geometrical material properties ========
# Light Collection efficiency
lightColl = cms.double(0.023),
# Light Collection uniformity
lightCollUnif = cms.double(0.003),
# Photostatistics (photons/GeV) in the homegeneous material
photoStatistics = cms.double(50.E3),
# Thickness of the detector in cm
thickness = cms.double(22.0),
#====== Global parameters of the material ========
# Interaction length in cm
interactionLength = cms.double(18.5),
Aeff = cms.double(170.87),
Zeff = cms.double(68.36),
rho = cms.double(8.280),
# Radiation length in g/cm^2
radLenIngcm2 = cms.double(7.37),
# ===== Those parameters might be entered by hand
# or calculated out of the previous ones
# Radiation length in cm. If value set to -1, FastSim uses internally the
# formula radLenIngcm2/rho
radLenIncm = cms.double(0.89),
# Critical energy in GeV. If value set to -1, FastSim uses internally the
# formula (2.66E-3*(x0*Z/A)^1.1): 8.74E-3 for ECAL EndCap
criticalEnergy = cms.double(8.74E-3),
# Moliere Radius in cm.If value set to -1, FastSim uses internally the
# formula : Es/criticalEnergy*X0 with Es=sqrt(4*Pi/alphaEM)*me*c^2=0.0212 GeV
# This value is known to be 2.190 cm for ECAL Endcap, but the formula gives 2.159 cm
moliereRadius = cms.double(2.190),
#====== Parameters for sampling ECAL ========
# Sampling Fraction: Fs = X0eff/(da+dp) where X0eff is the average X0
# of the active and passive media and da/dp their thicknesses
Fs = cms.double(0.0),
# e/mip for the calorimeter. May be estimated by 1./(1+0.007*(Zp-Za))
ehat = cms.double(0.0),
# a rough estimate of ECAL resolution sigma/E = resE/sqrt(E)
# it is used to generate Nspots in radial profiles.
resE = cms.double(1.),
# the width in cm of the active layer
da = cms.double(0.2),
# the width in cm of the passive layer
dp = cms.double(0.8),
# Is a homogenious detector?
bHom = cms.bool(True),
# Activate the LogDebug
debug = cms.bool(False)
)
),
Debug = cms.untracked.bool(False),
useDQM = cms.untracked.bool(False),
# EvtsToDebug = cms.untracked.vuint32(487),
HCAL = cms.PSet(
SimMethod = cms.int32(0), ## 0 - use HDShower, 1 - use HDRShower, 2 - GFLASH
GridSize = cms.int32(7),
#-- 0 - simple response, 1 - parametrized response + showering, 2 - tabulated response + showering
SimOption = cms.int32(2),
Digitizer = cms.untracked.bool(False),
samplingHBHE = cms.vdouble(125.44, 125.54, 125.32, 125.13, 124.46,
125.01, 125.22, 125.48, 124.45, 125.90,
125.83, 127.01, 126.82, 129.73, 131.83,
143.52, # HB
210.55, 197.93, 186.12, 189.64, 189.63,
190.28, 189.61, 189.60, 190.12, 191.22,
190.90, 193.06, 188.42, 188.42), #HE
samplingHF = cms.vdouble(0.383, 0.368),
samplingHO = cms.vdouble(231.0, 231.0, 231.0, 231.0, 360.0,
360.0, 360.0, 360.0, 360.0, 360.0,
360.0, 360.0, 360.0, 360.0, 360.0),
ietaShiftHB = cms.int32(1),
timeShiftHB = cms.vdouble(6.9, 6.9, 7.1, 7.1, 7.3, 7.5, 7.9, 8.3, 8.7, 9.1, 9.5, 10.3, 10.9, 11.5, 12.3, 14.1),
ietaShiftHE = cms.int32(16),
timeShiftHE = cms.vdouble(16.9, 15.7, 15.3, 15.3, 15.1, 14.9, 14.7, 14.7, 14.5, 14.5, 14.3, 14.3, 14.5, 13.9),
ietaShiftHO = cms.int32(1),
timeShiftHO = cms.vdouble(13.7, 13.7, 13.9, 14.1, 15.1, 15.7, 16.5, 17.3, 18.1, 19.1, 20.3, 21.9, 23.3, 25.5, 26.1),
ietaShiftHF = cms.int32(29),
timeShiftHF = cms.vdouble(50.7, 52.5, 52.9, 53.9, 54.5, 55.1, 55.1, 55.7, 55.9, 56.1, 56.1, 56.1, 56.5),
),
HFShower = cms.PSet(
HFShowerBlock = cms.PSet(refToPSet_ = cms.string("HFShowerBlock"))
),
HFShowerLibrary = cms.PSet(
useShowerLibrary = cms.untracked.bool(True),
useCorrectionSL = cms.untracked.bool(True),
ApplyFiducialCut = cms.bool(True),
HFLibraryFileBlock = cms.PSet(refToPSet_ = cms.string("HFLibraryFileBlock"))
)
),
GFlash = cms.PSet(
GflashExportToFastSim = cms.bool(True),
GflashHadronPhysics = cms.string('QGSP_BERT'),
GflashEMShowerModel = cms.bool(False),
GflashHadronShowerModel = cms.bool(True),
GflashHcalOuter = cms.bool(False),
GflashHistogram = cms.bool(False),
GflashHistogramName = cms.string('gflash_histogram.root'),
Verbosity = cms.untracked.int32(0),
bField = cms.double(3.8),
watcherOn = cms.bool(False),
tuning_pList = cms.vdouble()
)
)
FamosCalorimetryBlock.Calorimetry.ECAL.Digitizer = True
FamosCalorimetryBlock.Calorimetry.HCAL.Digitizer = True
from Configuration.Eras.Modifier_run2_common_cff import run2_common