Python implementation of the Raubold and Lynch method for n-body events using TensorFlow as a backend.
The code is based on the GENBOD function (W515 from CERNLIB), documented in [1] and tries to follow it as closely as possible.
Detailed documentation, including the API, can be found in https://phasespace.readthedocs.io. Don't hesitate to join our gitter channel for questions and comments.
If you use phasespace in a scientific publication we would appreciate citations to the JOSS publication:
@article{puig_eschle_phasespace-2019,
title = {phasespace: n-body phase space generation in Python},
doi = {10.21105/joss.01570},
url = {https://doi.org/10.21105/joss.01570},
year = {2019},
month = {oct},
publisher = {The Open Journal},
author = {Albert Puig and Jonas Eschle},
journal = {Journal of Open Source Software}
}Free software: BSD-3-Clause.
[1] F. James, Monte Carlo Phase Space, CERN 68-15 (1968)
Lately, data analysis in High Energy Physics (HEP), traditionally performed within the ROOT ecosystem, has been moving more and more towards Python. The possibility of carrying out purely Python-based analyses has become real thanks to the development of many open source Python packages, which have allowed to replace most ROOT functionality with Python-based packages.
One of the aspects where this is still not possible is in the random generation of n-body phase space events, which are widely used in the field, for example to study kinematics of the particle decays of interest, or to perform importance sampling in the case of complex amplitude models. This has been traditionally done with the TGenPhaseSpace class, which is based of the GENBOD function of the CERNLIB FORTRAN libraries and which requires a full working ROOT installation.
This package aims to address this issue by providing a TensorFlow-based implementation of such a function
to generate n-body decays without requiring a ROOT installation.
Additionally, an oft-needed functionality to generate complex decay chains, not included in TGenPhaseSpace,
is also offered, leaving room for decaying resonances (which don't have a fixed mass, but can be seen as a
broad peak).
To install with pip:
$ pip install phasespaceThis is the preferred method to install phasespace, as it will always install the most recent stable release.
To install the necessary dependencies to be used with
DecayLanguage, use
$ pip install "phasespace[fromdecay]"Phasespace can directly be used to generate from a DecayChain using the DecayLanguage package as explained in the tutorial.
The generation of simple n-body decays can be done using the nbody_decay shortcut to create a decay chain
with a very simple interface: one needs to pass the mass of the top particle and the masses of the children particle as
a list, optionally giving the names of the particles. Then, the generate method can be used to produce the desired sample.
For example, to generate B^0\to K\pi, we would do:
import phasespace
B0_MASS = 5279.65
PION_MASS = 139.57018
KAON_MASS = 493.677
weights, particles = phasespace.nbody_decay(B0_MASS,
[PION_MASS, KAON_MASS]).generate(n_events=1000)Behind the scenes, this function runs the TensorFlow graph. It returns tf.Tensor, which, as TensorFlow 2.x is in eager mode,
is basically a numpy array. Any tf.Tensor can be explicitly converted to a numpy array by calling tf.Tensor.numpy() on it.
The generate function returns a tf.Tensor of 1000 elements in the case of weights and a list of
n particles (2) arrays of (1000, 4) shape,
where each of the 4-dimensions corresponds to one of the components of the generated Lorentz 4-vector.
All particles are generated in the rest frame of the top particle; boosting to a certain momentum (or list of momenta) can be
achieved by passing the momenta to the boost_to argument.
Sequential decays can be handled with the GenParticle class (used internally by generate) and its set_children method.
As an example, to build the B^{0}\to K^{*}\gamma decay in which K^*\to K\pi, we would write:
from phasespace import GenParticle
B0_MASS = 5279.65
KSTARZ_MASS = 895.55
PION_MASS = 139.57018
KAON_MASS = 493.677
kaon = GenParticle('K+', KAON_MASS)
pion = GenParticle('pi-', PION_MASS)
kstar = GenParticle('K*', KSTARZ_MASS).set_children(kaon, pion)
gamma = GenParticle('gamma', 0)
bz = GenParticle('B0', B0_MASS).set_children(kstar, gamma)
weights, particles = bz.generate(n_events=1000)Where we have used the fact that set_children returns the parent particle.
In this case, particles is a dict with the particle names as keys:
>>> particles
{'K*': array([[ 1732.79325872, -1632.88873127, 950.85807735, 2715.78804872],
[-1633.95329448, 239.88921123, -1961.0402768 , 2715.78804872],
[ 407.15613764, -2236.6569286 , -1185.16616251, 2715.78804872],
...,
[ 1091.64603395, -1301.78721269, 1920.07503991, 2715.78804872],
[ -517.3125083 , 1901.39296899, 1640.15905194, 2715.78804872],
[ 656.56413668, -804.76922982, 2343.99214816, 2715.78804872]]),
'K+': array([[ 750.08077976, -547.22569019, 224.6920906 , 1075.30490935],
[-1499.90049089, 289.19714633, -1935.27960292, 2514.43047106],
[ 97.64746732, -1236.68112923, -381.09526192, 1388.47607911],
...,
[ 508.66157459, -917.93523639, 1474.7064148 , 1876.11771642],
[ -212.28646168, 540.26381432, 610.86656669, 976.63988936],
[ 177.16656666, -535.98777569, 946.12636904, 1207.28744488]]),
'gamma': array([[-1732.79325872, 1632.88873127, -950.85807735, 2563.79195128],
[ 1633.95329448, -239.88921123, 1961.0402768 , 2563.79195128],
[ -407.15613764, 2236.6569286 , 1185.16616251, 2563.79195128],
...,
[-1091.64603395, 1301.78721269, -1920.07503991, 2563.79195128],
[ 517.3125083 , -1901.39296899, -1640.15905194, 2563.79195128],
[ -656.56413668, 804.76922982, -2343.99214816, 2563.79195128]]),
'pi-': array([[ 982.71247896, -1085.66304109, 726.16598675, 1640.48313937],
[ -134.0528036 , -49.3079351 , -25.76067389, 201.35757766],
[ 309.50867032, -999.97579937, -804.0709006 , 1327.31196961],
...,
[ 582.98445936, -383.85197629, 445.36862511, 839.6703323 ],
[ -305.02604662, 1361.12915468, 1029.29248526, 1739.14815935],
[ 479.39757002, -268.78145413, 1397.86577911, 1508.50060384]])}The GenParticle class is able to cache the graphs so it is possible to generate in a loop without overhead:
for i in range(10):
weights, particles = bz.generate(n_events=1000)
...
(do something with weights and particles)
...This way of generating is recommended in the case of large samples, as it allows to benefit from parallelisation while at the same time keep the memory usage low.
If we want to operate with the TensorFlow graph instead, we can use the generate_tensor method of GenParticle, which has the same signature as generate.
More examples can be found in the tests folder and in the documentation.
Physics validation is performed continuously in the included tests (tests/test_physics.py), run through GitHub Actions.
This validation is performed at two levels:
- In simple n-body decays, the results of
phasespaceare checked againstTGenPhaseSpace. - For sequential decays, the results of
phasespaceare checked against RapidSim, a "fast Monte Carlo generator for simulation of heavy-quark hadron decays". In the case of resonances, differences are expected because our tests don't include proper modelling of their mass shape, as it would require the introduction of further dependencies. However, the results of the comparison can be expected visually.
The results of all physics validation performed by the tests_physics.py test are written in tests/plots.
Contributions are always welcome, please have a look at the Contributing guide.