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import FWCore.ParameterSet.Config as cms
# Material effects to be simulated in the tracker material and associated cuts
MaterialEffectsBlock = cms.PSet(
MaterialEffects = cms.PSet(
use_hardcoded_geometry = cms.bool(True),
# Material Properties (Silicon)
# A
A = cms.double(28.0855),
# Z
Z = cms.double(14.0),
# Density in g/cm3
Density = cms.double(2.329),
# One radiation length in cm
RadiationLength = cms.double(9.36),
# upper energy limit for the Bertini cascade
EkinBertiniGeV = cms.double(3.5),
# Kinetic energy threshold for secondaries
EkinLimitGeV = cms.double(0.1),
# General switches
# Enable photon pair conversion
PairProduction = cms.bool(True),
# Smallest photon energy allowed for conversion
photonEnergy = cms.double(0.1),
# Enable electron Bremsstrahlung
Bremsstrahlung = cms.bool(True),
# Enable muon Bremsstrahlung
MuonBremsstrahlung = cms.bool(False),
# Smallest bremstrahlung photon energy
bremEnergy = cms.double(0.1),
# Smallest bremsstrahlung energy fraction (wrt to the electron energy)
bremEnergyFraction = cms.double(0.005),
# Enable dE/dx
EnergyLoss = cms.bool(True),
# Enable Multiple Scattering
MultipleScattering = cms.bool(True),
# Smallest pT for the Mutliple Scattering
pTmin = cms.double(0.2),
# Enable Nuclear Interactions
NuclearInteraction = cms.bool(True), # buggy, should be removed on long term
#
G4NuclearInteraction = cms.bool(False),
# The energies of the pions used in the above files (same order)
hadronEnergies = cms.untracked.vdouble(
1.0, 2.0, 3.0, 4.0, 5.0, 7.0, 9.0, 12.0, 15.0, 20.0,
30.0, 50.0, 100.0, 200.0, 300.0, 500.0, 700.0, 1000.0
),
# The particle types simulated
hadronTypes = cms.untracked.vint32(
211, -211, 130, 321, -321, 2212, -2212, 2112, -2112
),
# The corresponding particle names
hadronNames = cms.untracked.vstring(
'piplus', 'piminus', 'K0L', 'Kplus', 'Kminus', 'p', 'pbar', 'n', 'nbar'
),
# The corresponding particle masses
hadronMasses = cms.untracked.vdouble(
0.13957, 0.13957, 0.497648, 0.493677, 0.493677,
0.93827, 0.93827, 0.939565, 0.939565
),
# The corresponding smallest momenta for which an inleatic interaction may occur
hadronMinP = cms.untracked.vdouble(
0.7, 0.0, 1.0, 1.0, 0.0, 1.1, 0.0, 1.1, 0.0
),
# The scaling of the inelastic cross section with energy
ratios = cms.untracked.vdouble(
# pi+ (211)
0.031390573,0.531842852,0.819614219,0.951251711,0.986382750,1.000000000,0.985087033,0.982996773,
0.990832192,0.992237923,0.994841580,0.973816742,0.967264815,0.971714258,0.969122824,0.978681792,
0.977312732,0.984255819,
# pi- (-211)
0.035326512,0.577356403,0.857118809,0.965683504,0.989659360,1.000000000,0.989599240,0.980665408,
0.988384816,0.981038152,0.975002104,0.959996152,0.953310808,0.954705592,0.957615400,0.961150456,
0.965022184,0.960573304,
# K0L (130)
0.000000000,0.370261189,0.649793096,0.734342408,0.749079499,0.753360057,0.755790543,0.755872164,
0.751337674,0.746685288,0.747519634,0.739357554,0.735004444,0.803039922,0.832749896,0.890900187,
0.936734805,1.000000000,
# K+ (321)
0.000000000,0.175571717,0.391683394,0.528946472,0.572818635,0.614210280,0.644125538,0.670304050,
0.685144573,0.702870161,0.714708513,0.730805263,0.777711536,0.831090576,0.869267129,0.915747562,
0.953370523,1.000000000,
# K- (-321)
0.000000000,0.365353210,0.611663677,0.715315908,0.733498956,0.738361302,0.745253654,0.751459671,
0.750628335,0.746442657,0.750850669,0.744895986,0.735093960,0.791663444,0.828609543,0.889993040,
0.940897842,1.000000000,
# proton (2212)
0.000000000,0.042849136,0.459103223,0.666165343,0.787930873,0.890397011,0.920999533,0.937832788,
0.950920131,0.966595049,0.979542270,0.988061653,0.983260159,0.988958431,0.991723494,0.995273237,
1.000000000,0.999962634,
# anti-proton (-2212)
1.000000000,0.849956907,0.775625988,0.802018230,0.816207485,0.785899785,0.754998487,0.728977244,
0.710010673,0.670890339,0.665627872,0.652682888,0.613334247,0.647534574,0.667910938,0.689919693,
0.709200185,0.724199928,
# neutron (2112)
0.000000000,0.059216484,0.437844536,0.610370629,0.702090648,0.780076890,0.802143073,0.819570432,
0.825829666,0.840079750,0.838435509,0.837529986,0.835687165,0.885205014,0.912450156,0.951451221,
0.973215562,1.000000000,
# anti-neutron
1.000000000,0.849573257,0.756479495,0.787147094,0.804572414,0.791806302,0.760234588,0.741109531,
0.724118186,0.692829761,0.688465897,0.671806061,0.636461171,0.675314029,0.699134460,0.724305037,
0.742556115,0.758504713
),
# The correspondence between long-lived hadrons/ions and the simulated hadron list
protons = cms.untracked.vint32(2212, 3222, -101, -102, -103, -104),
antiprotons = cms.untracked.vint32(-2212, -3222),
neutrons = cms.untracked.vint32(2112, 3122, 3112, 3312, 3322, 3334, -3334),
antineutrons = cms.untracked.vint32(-2112, -3122, -3112, -3312, -3322),
K0Ls = cms.untracked.vint32(130, 310),
Kplusses = cms.untracked.vint32(321),
Kminusses = cms.untracked.vint32(-321),
Piplusses = cms.untracked.vint32(211),
Piminusses = cms.untracked.vint32(-211),
# The smallest pion energy for which nuclear interactions are simulated
pionEnergy = cms.double(0.2),
# The algorihm to detrmine the distance between the primary and the secondaries
# 0 = no link
# 1 = sin(theta12) - ~ ok at all momenta
# 2 = sin(theta12) * p1/p2 - bad, should not be used
distAlgo = cms.uint32(1),
distCut = cms.double(0.020), ## Default is 0.020 for algo 1;
# The ratio between radiation lengths and interation lengths in the tracker at 15 GeV
lengthRatio = cms.vdouble(
# pi+ pi- K0L K+ K- p pbar n nbar
# 0.2508, 0.2549, 0.3380, 0.2879, 0.3171, 0.3282, 0.5371, 0.3859, 0.5086 # before 170 tuning
0.2257, 0.2294, 0.3042, 0.2591, 0.2854, 0.3101, 0.5216, 0.3668, 0.4898 # after 170 tuning
),
# and a global fudge factor for TEC Layers to make it fit
fudgeFactor = cms.double(1.2),
# The file with the last nuclear interaction read in the previous run
# to be put in the local running directory (if desired)
inputFile = cms.untracked.string('NuclearInteractionInputFile.txt'),
)
)
MaterialEffectsForMuonsBlock = cms.PSet(
MaterialEffectsForMuons = cms.PSet(
use_hardcoded_geometry = cms.bool(True),
#print hi
#print use_hardcoded_geometry
# Material Properties (Iron - this is for muons)
# A
A = cms.double(55.8455),
# Z
Z = cms.double(26.0),
# Density in g/cm3
Density = cms.double(7.87),
# One radiation length in cm
RadiationLength = cms.double(1.76),
# GEneral switches
# Enable photon pair conversion
PairProduction = cms.bool(False),
# Smallest photon energy allowed for conversion
photonEnergy = cms.double(0.1),
# Enable electron Bremsstrahlung
Bremsstrahlung = cms.bool(False),
# Enable muon Bremsstrahlung
MuonBremsstrahlung = cms.bool(False),
# Smallest bremstrahlung photon energy
bremEnergy = cms.double(0.1),
# Smallest bremsstrahlung energy fraction (wrt to the electron energy)
bremEnergyFraction = cms.double(0.005),
# Enable dE/dx
EnergyLoss = cms.bool(True),
# Enable Multiple Scattering
MultipleScattering = cms.bool(True),
# Smallest pT for the Mutliple Scattering
pTmin = cms.double(0.3),
# Enable Nuclear Interactions
G4NuclearInteraction = cms.bool(False),
NuclearInteraction = cms.bool(False)
)
)
MaterialEffectsForMuonsInECALBlock = cms.PSet(
MaterialEffectsForMuonsInECAL = cms.PSet(
use_hardcoded_geometry = cms.bool(True),
# Material Properties (PbW04 - this is for muons)
# A
A = cms.double(55.8455),
# Z
Z = cms.double(26.0),
# Density in g/cm3
Density = cms.double(8.280),
# One radiation length in cm
RadiationLength = cms.double(0.89),
# GEneral switches
# Enable photon pair conversion
PairProduction = cms.bool(False),
# Smallest photon energy allowed for conversion
photonEnergy = cms.double(0.1),
# Enable electron Bremsstrahlung
Bremsstrahlung = cms.bool(False),
# Enable muon Bremsstrahlung
MuonBremsstrahlung = cms.bool(False),
# Smallest bremstrahlung photon energy
bremEnergy = cms.double(0.1),
# Smallest bremsstrahlung energy fraction (wrt to the electron energy)
bremEnergyFraction = cms.double(0.005),
# Enable dE/dx
EnergyLoss = cms.bool(False),
# Enable Multiple Scattering
MultipleScattering = cms.bool(False),
# Smallest pT for the Mutliple Scattering
pTmin = cms.double(0.3),
# Enable Nuclear Interactions
G4NuclearInteraction = cms.bool(False),
NuclearInteraction = cms.bool(False)
)
)
MaterialEffectsForMuonsInHCALBlock = cms.PSet(
MaterialEffectsForMuonsInHCAL = cms.PSet(
use_hardcoded_geometry = cms.bool(True),
# Material Properties (BRASS - this is for muons)
# A
A = cms.double(64.0),
# Z
Z = cms.double(29.0),
# Density in g/cm3
Density = cms.double(8.5),
# One radiation length in cm
RadiationLength = cms.double(1.44),
# GEneral switches
# Enable photon pair conversion
PairProduction = cms.bool(False),
# Smallest photon energy allowed for conversion
photonEnergy = cms.double(0.1),
# Enable electron Bremsstrahlung
Bremsstrahlung = cms.bool(False),
# Enable muon Bremsstrahlung
MuonBremsstrahlung = cms.bool(False),
# Smallest bremstrahlung photon energy
bremEnergy = cms.double(0.1),
# Smallest bremsstrahlung energy fraction (wrt to the electron energy)
bremEnergyFraction = cms.double(0.005),
# Enable dE/dx
EnergyLoss = cms.bool(False),
# Enable Multiple Scattering
MultipleScattering = cms.bool(False),
# Smallest pT for the Mutliple Scattering
pTmin = cms.double(0.3),
# Enable Nuclear Interactions
G4NuclearInteraction = cms.bool(False),
NuclearInteraction = cms.bool(False)
)
)
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