Evaluation of G4 Releases in CMS (Sub-detector Studies) Software used Electrons in Tracker Photons in the Electromagnetic Calorimeter Pions in the Calorimeter.

Slides:



Advertisements
Similar presentations
CBM Calorimeter System CBM collaboration meeting, October 2008 I.Korolko(ITEP, Moscow)
Advertisements

Particle identification in ECAL Alexander Artamonov, Yuri Kharlov IHEP, Protvino CBM collaboration meeting
Use of G EANT 4 in CMS AIHENP’99 Crete, April 1999 Véronique Lefébure CERN EP/CMC.
LC Calorimeter Testbeam Requirements Sufficient data for Energy Flow algorithm development Provide data for calorimeter tracking algorithms  Help setting.
April 19th, 2010Philippe Doublet (LAL) Hadronic showers in the SiW ECAL (with 2008 FNAL data) Philippe Doublet.
The performance of Strip-Fiber EM Calorimeter response uniformity, spatial resolution The 7th ACFA Workshop on Physics and Detector at Future Linear Collider.
INTRODUCTION TO e/ ɣ IN ATLAS In order to acquire the full physics potential of the LHC, the ATLAS electromagnetic calorimeter must be able to identify.
W. Clarida, HCAL Meeting, Fermilab Oct. 06 Quartz Plate Calorimeter Prototype Geant4 Simulation Progress W. Clarida The University of Iowa.
ECAL Spike Plot Approval ECAL Anomalous Signal Plots Approval Adi Bornheim for ECAL
First CMS Results with LHC BeamToyoko Orimoto, Caltech 1 First CMS Results with LHC Beam Toyoko Orimoto California Institute of Technology On behalf of.
Calorimeter1 Understanding the Performance of CMS Calorimeter Seema Sharma,TIFR (On behalf of CMS HCAL)
1Calice-UK Cambridge 9/9/05D.R. Ward David Ward Compare Feb’05 DESY data with Geant4 and Geant3 Monte Carlos. Work in progress – no definitive conclusions.
 Performance Goals -> Motivation  Analog/Digital Comparisons  E-flow Algorithm Development  Readout R&D  Summary Optimization of the Hadron Calorimeter.
A preliminary analysis of the CALICE test beam data Dhiman Chakraborty, NIU for the CALICE Collaboration LCWS07, Hamburg, Germany May 29 - June 3, 2007.
1 Calice Analysis Meeting 13/02/07David Ward Just a collection of thoughts to guide us in planning electron analysis In order to end up with a coherent.
1/9/2003 UTA-GEM Simulation Report Venkatesh Kaushik 1 Simulation Study of Digital Hadron Calorimeter Using GEM Venkatesh Kaushik* University of Texas.
Application of Neural Networks for Energy Reconstruction J. Damgov and L. Litov University of Sofia.
Track Extrapolation/Shower Reconstruction in a Digital HCAL – ANL Approach Steve Magill ANL 1 st step - Track extrapolation thru Cal – substitute for Cal.
Presentation Title Spike problem.
Progress with the Development of Energy Flow Algorithms at Argonne José Repond for Steve Kuhlmann and Steve Magill Argonne National Laboratory Linear Collider.
1 HCAL Upgrade TP simulation studies Jane Nachtman (Iowa) – for the HCAL group Trigger Upgrade meeting April 28, 2010.
Geant4 Acceptance Suite for Key Observables CHEP06, T.I.F.R. Mumbai, February 2006 J. Apostolakis, I. MacLaren, J. Apostolakis, I. MacLaren, P. Mendez.
Readiness of CMS Simulation towards LHC Startup Outline  Introduction  Framework and Interface with GEANT4  Detector specific components  How have.
CHEP 2006 D. Elvira, M. Stavrianakou, FNAL 1 The CMS Object-Oriented Simulation V. Daniel Elvira and Maya Stavrianakou, FNAL On behalf of the CMS collaboration.
Implementing a dual readout calorimeter in SLIC and testing Geant4 Physics Hans Wenzel Fermilab Friday, 2 nd October 2009 ALCPG 2009.
CHEP06, Mumbai-India, Feb 2006V. Daniel Elvira 1 The CMS Simulation Validation Suite V. Daniel Elvira (Fermilab) for the CMS Collaboration.
Event Reconstruction in SiD02 with a Dual Readout Calorimeter Detector Geometry EM Calibration Cerenkov/Scintillator Correction Jet Reconstruction Performance.
Hadron energy reconstruction in ATLAS Ongoing work (Per, Kerstin and C Santoni and V Giangiobbe from C-F): Analysis of combined test beam data: reconstruction.
26 Apr 2009Paul Dauncey1 Digital ECAL: Lecture 1 Paul Dauncey Imperial College London.
LHCb production experience with Geant4 LCG Applications Area Meeting October F.Ranjard/ CERN.
Release Validation J. Apostolakis, M. Asai, G. Cosmo, S. Incerti, V. Ivantchenko, D. Wright for Geant4 12 January 2009.
Development of a Particle Flow Algorithms (PFA) at Argonne Presented by Lei Xia ANL - HEP.
January 21, 2007Suvadeep Bose / IndiaCMS - Santiniketan 1 Response of CMS Hadron Calorimeter to Electron Beams Suvadeep Bose EHEP, TIFR, Mumbai Outline:
UTA GEM DHCAL Simulation Jae Yu * UTA DoE Site Visit Nov. 13, 2003 (*On behalf of the UTA team; A. Brandt, K. De, S. Habib, V. Kaushik, J. Li, M. Sosebee,
The CMS Simulation Software Julia Yarba, Fermilab on behalf of CMS Collaboration 22 m long, 15 m in diameter Over a million geometrical volumes Many complex.
ECAL PID1 Particle identification in ECAL Yuri Kharlov, Alexander Artamonov IHEP, Protvino CBM collaboration meeting
CMS H4 ECAL testbeam data comparison with simulation F.Cossutti a), B. Heltsey b), P. Meridiani c), C. Rovelli c) a) INFN Trieste b) Cornell University.
1ECFA/Vienna 16/11/05D.R. Ward David Ward Compare these test beam data with Geant4 and Geant3 Monte Carlos. CALICE has tested an (incomplete) prototype.
PHOTON RECONSTRUCTION IN CMS APPLICATION TO H   PHOTON RECONSTRUCTION IN CMS APPLICATION TO H   Elizabeth Locci SPP/DAPNIA, Saclay, France Prague.
Bangalore, India1 Performance of GLD Detector Bangalore March 9 th -13 th, 2006 T.Yoshioka (ICEPP) on behalf of the.
1 QuickSim - brief introduction - Akiya Miyamoto KEK 22 June 2005 GLD meeting See also.
13 July 2005 ACFA8 Gamma Finding procedure for Realistic PFA T.Fujikawa(Tohoku Univ.), M-C. Chang(Tohoku Univ.), K.Fujii(KEK), A.Miyamoto(KEK), S.Yamashita(ICEPP),
The experimental setup of Test Beam HE EE ES BEAM  A slice of the CMS calorimter was tested during summer of 2007 at the H2 test beam area at CERN with.
Fast Shower Simulation in ATLAS Calorimeter Wolfgang Ehrenfeld – University of Hamburg/DESY On behalf of the Atlas-Calorimeter and Atlas-Fast-Parameterisation.
Status of Reconstruction in sidloi3 Ron Cassell 5/20/10.
First CMS Results with LHC Beam
Geant4 CPU performance : an update Geant4 Technical Forum, CERN, 07 November 2007 J.Apostolakis, G.Cooperman, G.Cosmo, V.Ivanchenko, I.Mclaren, T.Nikitina,
1 Hadronic calorimeter simulation S.Itoh, T.Takeshita ( Shinshu Univ.) GLC calorimeter group Contents - Comparison between Scintillator and Gas - Digital.
Individual Particle Reconstruction The PFA Approach to Detector Development for the ILC Steve Magill (ANL) Norman Graf, Ron Cassell (SLAC)
1 IWLC 2010 Geneva Oct.’10David Ward Tests of GEANT4 using the CALICE calorimeters David Ward  Electromagnetic particles (, e) were used to understand.
Validation of Geant4 (V4.2) for GLAST-LAT -Comparison with Theory, Beam Test Data and EGS4 – S. Ogata, T. Mizuno, H. Mizushima (Hiroshima/SLAC) P. Valtersson,
1 Plannar Active Absorber Calorimeter Adam Para, Niki Saoulidou, Hans Wenzel, Shin-Shan Yu Fermialb Tianchi Zhao University of Washington ACFA Meeting.
2005/07/12 (Tue)8th ACFA Full simulator study of muon detector and calorimeter 8th ACFA Workshop at Daegu, Korea 2005/07/12 (Tue) Hiroaki.
Photon & e+e- Hits in Muon Higgs Factory T. Markiewicz T. Maruyama SLAC MAP Collaboration Meeting. Fermilab 29 May 2014.
ECAL Interaction layer PFA Template Track/CalCluster Association Track extrapolation Mip finding Shower interaction point Shower cluster pointing Shower.
Lecture 18 - Detectors Detector systems
Dual Readout Clustering and Jet Finding
CALICE scintillator HCAL
Simulation Project Structure and tasks
of experiment simulations
Physics Validation of LHC Simulations
Individual Particle Reconstruction
CMS-Bijing weekly meeting
Comparison between Geant4, Fluka and the TileCal test-beam data
Argonne National Laboratory
Backgrounds using v7 Mask in 9 Si Layers at a Muon Higgs Factory
Status of CEPC HCAL Optimization Study in Simulation LIU Bing On behalf the CEPC Calorimeter working group.
Steve Magill Steve Kuhlmann ANL/SLAC Motivation
LC Calorimeter Testbeam Requirements
CMS-Bijing weekly meeting
Presentation transcript:

Evaluation of G4 Releases in CMS (Sub-detector Studies) Software used Electrons in Tracker Photons in the Electromagnetic Calorimeter Pions in the Calorimeter System S. Banerjee, TIFR/CERN (on behalf of CMS simulation team) LCG Validation Meeting October 25, 2006

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 2 Software Used Tracker, Electromagnetic Calorimeter and Combined Calorimeter system all use CMSSW version 0_8_1 for Geant4.7.1.p02 with some CMS specific changes For Geant4.8.1.p01, all sub-detector systems use CMSSW version 0_9_0_pre2 The different versions of CMSSW differ very little in handling hits and are identical in geometry Tracker and electromagnetic calorimeter studies use standard CMS detector for the geometry. The studies for the π showers use geometry of the calorimeter system only. Production cuts used are default CMS – typically 0.01 mm in pixel detector, 0.1 mm in tracker and pre-shower detectors, 1 mm in most parts of the detector Tests are run on 3.6 GHz dual processor with 4GB memory

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 3 Electrons in Tracker Geometry used : Entire CMS detector Event sample: 2000 electron events 20 GeV electrons generated with ІηІ < 3.5 and –π ≤ φ ≤ π Geant QGSP sample was generated on a 3.2 GHz processor with 2 GB memory Process used: Particle Gun + Vertex Smear + G4 SimHit Geant p02QGSP sec/event Geant p01QGSP sec/event Geant p01QGSP_EMV2.7 sec/event

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 4 Tracker Hit Comparison The hit quantities are similar in all the versions

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 5 Tracker Hits Geant QGSP shows slightly wider distribution in the Δz distributions Geant gives more secondary hits than the new version. QGSP_EMV has a mean somewhere in between

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 6 Samples and Physics list Geometry used: –Entire CMS detector Samples used in tests: – Particle Gun –10000 Photon: η=0.2, -π ≤ φ≤ π, E=30 GeV. –10000 Photon: η=2.2, -π ≤ φ≤ π, E=30 GeV. Physics List used in tests –Geant4.7.1_QGSP with CMSSW_0_8_1. –Geant4.8.1_QGSP with CMSSW_0_9_0_pre2_g4_81 –Geant4.8.1_QGSP_EMV with CMSSW_0_9_0_pre2_g4_81

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 7 Energy deposited in 1x1 Cluster in EB Geant471_QGSP is close to G481_QGSP_EMV Obvious difference between G471_QGSP and G481_QGSP –G471_QGSP gives the largest Energy deposition (mean= GeV) –G481_QGSP gives the smallest energy deposition (mean = GeV)

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 8 Energy deposited in 5x5 Cluster in EB Geant471_QGSP is very close to G481_QGSP_EMV Obvious difference between G471_QGSP and G481_QGSP –G471_QGSP gives the largest energy deposition (mean= GeV) –G481_QGSP gives the smallest energy deposition (mean = GeV)

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 9 Cluster Ratio in Barrel G471_QGSP: E1/E25 = G481_QGSP_EMV: E1/E25 = G481_QGSP: E1/E25 =0.6905

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 10 Percentage of energy deposited in EB E Inci =30 GeV: Energy of incident particle. E Barrel : Energy deposited in Barrel. G481_QGSP_EMV: 98.46% G471_QGSP: 98.39% G481_QGSP: 98.34% (smallest)

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 11 Percentage of energy deposited in EE E Inci =30 GeV: Energy of incident particle. E endcap : Energy deposited in Endcap. G481_QGSP_EMV: 95.45% G471_QGSP: 95.48% G481_QGSP: 95.25% (smallest)

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 12 Energy Deposit in 1 st Layer of PreShower. The average energy of hits in Preshower: –G471_QGSP: MeV –G481_QGSP_EMV: MeV –G481_QGSP: MeV

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 13 # Hits in the 2 nd layer of Preshower The Average Hit Number in the 2 nd Layer: –G471_QGSP: –G481_QGSP_EMV: –G481_QGSP: 9.72

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 14 Percentage of energy deposited in ES Total energy deposited in the preshower detector is consistent among the 3 physics lists.

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 15 Pions in the Calorimeter Geometry used : Electromagnetic and Hadron calorimeter Event sample: 2000 pion events 100 GeV pions generated separately in the barrel (ІηІ ≈ 0.3) and the endcap (ІηІ ≈ 2.1) detectors with in a small φ window Process used: Particle Gun + Vertex Smear + G4 SimHit Geant VersionPhysics ListBarrelEndcap p02QGSP sec/event7.44 sec/event p01QGSP sec/event10.19 sec/event p01QGSP_EMV8.56 sec/event7.29 sec/event

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 16 Energy measured in HB and HE Geant shows larger energy measurement (in particular the one with standard EM physics) Barrel and endcap show similar patterns

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 17 Hit Energy in HB and HE Geant shows softer spectrum for energy of individual hits This is a bit more pronounced with standard EM physics

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 18 Longitudinal Shower Profile The samples with Geant show larger energy deposit in earlier layers but energy deposit in later layers are similar This enhancement is more pronounced with QGSP 3.1 Barrel and endcap show similar patterns

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 19 Number of Hits There are more hits in ECal as well as in HCal in the Geant version A similar trend is observed for the endcap (not shown)

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 20 Time Profile of Hits The extra hits in Geant appear at a later time After energy weighting the time profiles are similar

25/10/2006 LCG-ValidationEvaluation of G4 releases in CMSS. Banerjee 21 Summary and Outlook Tracker sees fewer hits in the version for electrons (more study is being done to understand what happens) Transverse shower profile for photons in crystals is similar between QGSP 2.8 (4.7.1) and QGSP_EMV (4.8.1). QGP 3.1 (4.8.1) shows slightly broader profile Longitudinal shower profile for hadrons show larger energy deposit at smaller depth but energy deposits at larger depths are similar Hit multiplicity in the showers increase (for both photons and pions). Average hit energy is smaller in the new version. The extra hits appear more at later time CMS has collected data with identified particle beams in 2006 and these data will be used to tune Geant4 physics in coming months