Smearing of particles by a toy detector
Code: "toy_detector.py". Programming language: Python
DMelt Version 1.4. Last modified: 02/07/1973. License: Free
https://datamelt.org/code/cache/toy_detector_3441.py
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# This is a toy example illustrating a detector response.
# It creates a random list of particles. Each particle characterized with 4 values (PT,ETA,PHI,MASS)
# (truth-level). Then it applies some detector smearing and loses to mimic a typical detector
# ------------
# How to debug:
# ------------
# Run inside DataMelt
# @author S.Chekanov (ANL)
import random
from math import *
from java.awt import Color
pi=3.14159
#datamelt debug: fill resolution histograms
#-----------------------------------------
from jhplot import *
c1 = HPlot()
c1.visible(True)
c1.setRangeX(0.6,1.4)
c1.setNameX("pT_{rec} / pT_{true}")
h1 = H1D("pT<100 GeV",100, -2, 2.0)
h2 = H1D("pT>1000 GeV",100, -2, 2.0)
#-----------------------------------------
# total number of collision events
NrOfEvents=10000
#################################################
# smearing for energies of jets or particles
#################################################
RESPONSE=0.98 # on average, energies are shifted by -2%
# suggested variations: (-2%, 2%)
# In addition, energies are stochastically smeared by a detector
# using this formula: sigma = B*E+A*sqrt(E)
# Note: positions are smeared with sigma x10 smaller
# Smearing for jets: (photons have A=0.1, B=0.0)
A=0.50 # stochastic term of a detector smearing for jet
B=0.03 # constant term of detector smearing
# Suggested variations:
# RESPONSE: 0.95-1.0
# A: 0.6-0.02
# B: 0.01-0.03
# simulate efficiency of some "bad" region in Eta (pseudorapidity)
# assume 80% efficiency for |Eta|>2.5
# in addition, |Eta|>2.5 has larger resolution (by a factor 3). See below.
Efficiency=0.8
# input: v - value to be smeared
# pt - the value to be smeared usually depends on energy (pT)
# scale - scale factor. For photons, electrons, muons, set to 0.1
def getSmear(v,pt,scale=1):
"""Apply some detector smearing and shift true value v"""
global A,B,RESPONSE
# assume constant B and stochastic A terms
sigma=scale*(B*pt+A*sqrt(pt))
return random.gauss(v*RESPONSE, sigma)
# create events with particles for each event:
for nev in xrange(NrOfEvents):
tot_particles=int(abs(random.gauss(mu=50, sigma=20))) # number of particles per event is taken at random
PT,ETA,PHI,MASS=[],[],[],[]
# create physics lists with particles characterized by pt, eta, phi, mass
# mimic initial physics distributions
for i in range(tot_particles):
PT.append(abs(random.gauss(mu=0, sigma=2000)))
ETA.append(random.uniform(-3, 3))
PHI.append(random.uniform(-pi, pi))
MASS.append(abs(random.gauss(mu=100, sigma=200)))
##########################################################
## start simulation of detector response.
##########################################################
PT_D=[]
ETA_D=[]
PHI_D=[]
MASS_D=[]
for i in xrange(tot_particles):
pt =getSmear(PT[i],PT[i])
mass=getSmear(MASS[i],PT[i])
eta =getSmear(ETA[i],PT[i],0.1) # positions are always x10 better measured
phi =getSmear(PHI[i],PT[i],0.1)
# First remove some particles in eta detector region with low efficiency
if (abs(eta)>2.5): # positive eta>2.5 has low efficiency (missing detector module)
eta =getSmear(ETA[i],PT[i],0.3) # x3 larger smearing
if (random.random()>Efficiency): continue;
PT_D.append(pt)
ETA_D.append(eta)
PHI_D.append(phi)
MASS_D.append(mass)
# datamelt debug: fill histogram
if (PT[i]<100): h1.fill(pt/PT[i])
if (PT[i]>1000): h2.fill(pt/PT[i])
if (nev%1000==0):
print "Physics event=",nev," has ",tot_particles," particles. After detector=",len(PT_D)
# OUTPUT:
# PT[], ETA[], PHI[], MASS[] - list of particles entering a detector
# PT_D[], ETA_D[], PHI_D[], MASS_D[] - list of particles after the detector
#-----------------------------------
# datamelt debug: show histogram
h1.setFill(True)
h1.setFillColor(Color.red)
h1.setColor(Color.red)
c1.draw(h1.getDensity())
h2.setFill(True)
h2.setFillColor(Color.blue)
h2.setColor(Color.blue)
c1.draw(h2.getDensity())
#-----------------------------------