LCG Meeting, May 14th 2003 V. Daniel Elvira1 G4 (OSCAR_1_4_0) Validation of CMS HCal V. Daniel Elvira Fermilab.

Slides:



Advertisements
Similar presentations
LC Calorimeter Testbeam Requirements Sufficient data for Energy Flow algorithm development Provide data for calorimeter tracking algorithms  Help setting.
Advertisements

Electromagnetic shower in the AHCAL selection criteria data / MonteCarlo comparison of: handling linearity shower shapes CALICE collaboration meeting may.
HCAL TB2002 CPT Week, CERN, 05-Nov-2002, S.Kunori1 HB TB2002 Some Results Shuichi Kunori Jordan Damgov 05-Nov-2002.
CMS Outer Hadron Calorimeter (HO) Project Naba K Mondal Tata Institute, Mumbai, India.
W. Clarida, HCAL Meeting, Fermilab Oct. 06 Quartz Plate Calorimeter Prototype Geant4 Simulation Progress W. Clarida The University of Iowa.
Calorimeter1 Understanding the Performance of CMS Calorimeter Seema Sharma,TIFR (On behalf of CMS HCAL)
Testbeam Requirements for LC Calorimetry S. R. Magill for the Calorimetry Working Group Physics/Detector Goals for LC Calorimetry E-flow implications for.
First CMS Results with LHC BeamToyoko Orimoto, Caltech 1 First CMS Results with LHC Beam Toyoko Orimoto California Institute of Technology On behalf of.
1 Measurement of f D + via D +   + Sheldon Stone, Syracuse University  D o D o, D o  K -  + K-K- K+K+ ++  K-K- K+K+ “I charm you, by my once-commended.
1 EMCal design MICE collaboration meeting Fermilab Rikard Sandström.
Michele Faucci Giannelli TILC09, Tsukuba, 18 April 2009 SiW Electromagnetic Calorimeter Testbeam results.
Evaluation of G4 Releases in CMS (Sub-detector Studies) Software used Electrons in Tracker Photons in the Electromagnetic Calorimeter Pions in the Calorimeter.
Study of a Compensating Calorimeter for a e + e - Linear Collider at Very High Energy 30 Aprile 2007 Vito Di Benedetto.
Intercalibration of the CMS Electromagnetic Calorimeter Using Neutral Pion Decays 1 M. Gataullin (California Institute of Technology) on behalf of the.
Study of response uniformity of LHCb ECAL Mikhail Prokudin, ITEP.
Interactions of pions in the Si-W ECAL prototype Towards a paper Naomi van der Kolk.
Preliminary comparison of ATLAS Combined test-beam data with G4: pions in calorimetric system Andrea Dotti, Per Johansson Physics Validation of LHC Simulation.
Jet Energy Scale at CMS Anwar A Bhatti June 8, 2006 XII International Conference on Calorimetry Chicago IL, USA.
CHEP06, Mumbai-India, Feb 2006V. Daniel Elvira 1 The CMS Simulation Validation Suite V. Daniel Elvira (Fermilab) for the CMS Collaboration.
Marco Delmastro 23/02/2006 Status of LAr EM performance andmeasurements fro CTB1 Status of LAr EM performance and measurements for CTB Overview Data -
Calibration of the CMS Electromagnetic Calorimeter with first LHC data
Pion Showers in Highly Granular Calorimeters Jaroslav Cvach on behalf of the CALICE Collaboration Institute of Physics of the ASCR, Na Slovance 2, CZ -
Kati Lassila-Perini/HIP HIP CMS Software and Physics project evaluation1/ Electron/ physics in CMS Kati Lassila-Perini HIP Activities in the.
1 Energy loss correction for a crystal calorimeter He Miao Institute of High Energy Physics Beijing, P.R.China.
January 21, 2007Suvadeep Bose / IndiaCMS - Santiniketan 1 Response of CMS Hadron Calorimeter to Electron Beams Suvadeep Bose EHEP, TIFR, Mumbai Outline:
May 1-3, LHC 2003V. Daniel Elvira1 CMS: Hadronic Calorimetry & Jet/ Performance V. Daniel Elvira Fermilab.
Feb. 7, 2007First GLAST symposium1 Measuring the PSF and the energy resolution with the GLAST-LAT Calibration Unit Ph. Bruel on behalf of the beam test.
08-June-2006 / Mayda M. VelascoCALOR Chicago1 Initial Calibration for the CMS Hadronic Calorimeter Barrel Mayda M. Velasco Northwestern University.
Apollo Go, NCU Taiwan BES III Luminosity Monitor Apollo Go National Central University, Taiwan September 16, 2002.
W-DHCAL Analysis Overview José Repond Argonne National Laboratory.
© Imperial College LondonPage 1 Tracking & Ecal Positional/Angular Resolution Hakan Yilmaz.
ECAL PID1 Particle identification in ECAL Yuri Kharlov, Alexander Artamonov IHEP, Protvino CBM collaboration meeting
G4 Validation meeting (5/11/2003) S.VIRET LPSC Grenoble Photon testbeam Data/G4 comparison  Motivation  Testbeam setup & simulation  Analysis & results.
Results from particle beam tests of the ATLAS liquid argon endcap calorimeters Beam test setup Signal reconstruction Response to electrons  Electromagnetic.
SCECAL progress report Tohru Takeshita (Shinshu) _DESY Beam Test summary _improvements for FNAL BT _FNAL module _current status at Fermilab.
PHOTON RECONSTRUCTION IN CMS APPLICATION TO H   PHOTON RECONSTRUCTION IN CMS APPLICATION TO H   Elizabeth Locci SPP/DAPNIA, Saclay, France Prague.
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.
Min-DHCAL: Measurements with Pions Benjamin Freund and José Repond Argonne National Laboratory CALICE Collaboration Meeting Max-Planck-Institute, Munich.
FSC Status and Plans Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group PANDA Russia workshop, ITEP 27 April 2010.
R.S. Orr 2009 TRIUMF Summer Institute
First CMS Results with LHC Beam
US CMS UC Riverside, 18-May-2001, S.Kunori1 Status of JetsMET Shuichi Kunori U. of Maryland 18-May-2001 PRS: Physics Reconstruction and Selection.
5-9 June 2006Erika Garutti - CALOR CALICE scintillator HCAL commissioning experience and test beam program Erika Garutti On behalf of the CALICE.
H C A L 11 th International Conference on Advanced Technology and Particle Physics Villa Olmo (Como - Italy), October 5 - 9, 2009 THE PERFORMANCE OF THE.
Longitudinal shower profile - CERN electron runs Valeria Bartsch University College London.
Calice Meeting Argonne Muon identification with the hadron calorimeter Nicola D’Ascenzo.
Geant4 Tutorial, Oct28 th 2003V. Daniel Elvira Geant4 Simulation of the CMS 2002 Hcal Test Beam V. Daniel Elvira Geant4 Tutorial.
 0 life time analysis updates, preliminary results from Primex experiment 08/13/2007 I.Larin, Hall-B meeting.
Test Beam Results on the ATLAS Electromagnetic Calorimeters Lucia Di Ciaccio – LAPP Annecy (on behalf of the ATLAS LAr Group) OUTLINE Description of the.
Régis Lefèvre (LPC Clermont-Ferrand - France)ATLAS Physics Workshop - Lund - September 2001 In situ jet energy calibration General considerations The different.
Feb. 3, 2007IFC meeting1 Beam test report Ph. Bruel on behalf of the beam test working group Gamma-ray Large Area Space Telescope.
Energy Reconstruction in the CALICE Fe-AHCal in Analog and Digital Mode Fe-AHCal testbeam CERN 2007 Coralie Neubüser CALICE Collaboration meeting Argonne,
1 Cosmic Ray Physics with IceTop and IceCube Serap Tilav University of Delaware for The IceCube Collaboration ISVHECRI2010 June 28 - July 2, 2010 Fermilab.
Quark Matter 2002, July 18-24, Nantes, France Dimuon Production from Au-Au Collisions at Ming Xiong Liu Los Alamos National Laboratory (for the PHENIX.
Zvi Citron Correlations Between Neutral Bosons and Jets in Pb+Pb Collisions at 2.76 TeV with the ATLAS Detector Zvi Citron for the ATLAS Collaboration.
A Study on Leakage and Energy Resolution
on behalf of ATLAS LAr Endcap Group
LKr inefficiency measurement
CALICE scintillator HCAL
Panagiotis Kokkas Univ. of Ioannina
CMS ECAL Calibration and Test Beam Results
Testbeam comparisons arXiv:
Physics Validation of LHC Simulations
HCAL – SiPM upgrade requirements
Scintillator HCAL: LOI issues
Kazuya Aoki For the PHENIX Collaborations. Kyoto Univ. / RIKEN
Michele Faucci Giannelli
Tests of a Digital Hadron Calorimeter
LC Calorimeter Testbeam Requirements
Presentation transcript:

LCG Meeting, May 14th 2003 V. Daniel Elvira1 G4 (OSCAR_1_4_0) Validation of CMS HCal V. Daniel Elvira Fermilab

LCG Meeting, May 14th 2003 V. Daniel Elvira2 General Description Simulate HCal test beam 2002 setup using OSCAR_1_4_0, physics list 1.8 Includes beam line (trigger scint. tiles, wire chambers), ECal box, HB, HO, aluminium slab (representing magnet), iron (muon) layer Mimic the data analysis, including calibration from electrons (ECal) and pions (HB): study resolution, response (linearity), transverse shower profiles Compare with data measurements for G4 validation

LCG Meeting, May 14th 2003 V. Daniel Elvira3 ECal 7x7 Crystal Matrix (movable) 2 HCal HB Modules HO Panels Aluminum Slab HCal 2002 Test Beam beam Moving table Small scale experiment to demonstrate that HCal works: 49 ECal crystals, 144 HB channels, 16 HO channels. Over 100 Million Events!  - : 225 GeV e - : 20,30,50,100 GeV  - : 20,30,50,100, 300 GeV

LCG Meeting, May 14th 2003 V. Daniel Elvira4     Based on 1-5,000   events onto the (  )=(6,2) tower of the HB and crystal 25 of the ECal matrix TB02 Simulation ( OSCAR/G4 ) Crystal 25

LCG Meeting, May 14th 2003 V. Daniel Elvira5 Angle view of the full TB02 detector 10 GeV electron HB ECal HO Beam Line HO HB ECal Beam Line TB02 Simulation ( OSCAR/G4 ) 100 GeV pion

LCG Meeting, May 14th 2003 V. Daniel Elvira6 E  corr = 122*E HB 5x *E ECal 3x3 E HB scint E HB scint + 0.1* E HB scint MeV * Rand E HB tower E HB tower MeV * Rand Long. Non-uniformity Electronic Noise Calibration factors (already there in previous presentation) E ECal tower E ECal tower +  match * Rand (To match the measured electron resolution-much worse than M.C.) Add more energy points at 10, 25, 200, 250, 300 GeV (in addition to 20, 30, 50, 100, 150 GeV) 5 times more statistics GeV Improved M.C. Simulation

LCG Meeting, May 14th 2003 V. Daniel Elvira7  /E=30.9% (similar to the fit to ¾ of second peak by Jordan) Data analysis: sources systematic errors: muon (pion decay) & electrons (from scrapping?) backgrounds calibration Data Analysis

LCG Meeting, May 14th 2003 V. Daniel Elvira8 From J.Damgov Electron background Muon background Background subtracted muon peak It should be possible to estimate background subtraction error by defining a band limited by an “aggressive” (bckgnd rejection) and a “conservative cut” (signal efficiency) The resolution comes down from 31% to 26.7% ! Pion Signal TB02:   E /E and e/ 

LCG Meeting, May 14th 2003 V. Daniel Elvira9 Pion peak Muon background Background subtracted pion peak  E /E = 20.3% TB02:   E /E and e/  50 GeV pions Pions showering in the crystals Data energy resolution for 50 GeV pions (almost negligible background close to the pion peak)

LCG Meeting, May 14th 2003 V. Daniel Elvira10 TB02:   E /E and e/  The agreement is excellent in all the energy range Shape difference: e/h (e.m. & nuclear x-sec), leakage……? Data systematic error analysis in progress Validate GEANT4 physics models Resolution Linearity

LCG Meeting, May 14th 2003 V. Daniel Elvira11 Transverse Shower Profile Future: remove ECal, add integrated profiles, longitud. profile studies, HO fraction & compare with OSCAR CMS & CMSIM (Salavat), and TB data (Jordan) G4/OSCAR TB02 crystals HB towers Fill ( D, E ) With D: distance of crystal/tower to the pion direction E: energy deposition

LCG Meeting, May 14th 2003 V. Daniel Elvira12 TB02 OSCAR_1_4_0 fully functional. Validation studies in progress, for week data uncertainties are essential. Need to port the simulation to OSCAR_2, hopefully for next CMS week in June fighting technical problems related to translation to XML, among other things Document on TB02 M.C. simulation by July Summary & Plans

LCG Meeting, May 14th 2003 V. Daniel Elvira13 Data & MC Electron Resolution 2.6% at 100 GeV for 3x3 tower matrix 2.8% at 100 GeV for 3x3 tower matrix E ECal tower E ECal tower MeV * Rand Electronic noise M.C resol much lower than measurement

LCG Meeting, May 14th 2003 V. Daniel Elvira14 E ECal tower E ECal tower MeV * Rand (noise) 2.3%/ sqrt(E ele ) (photo-statistics) 0.3% (longitudinal non-uniformity) 0.4% (calibration) Other Contributions No significant change E ECal tower E ECal tower +  match * Rand (To match the measured electron resolution) Temperature  R esp =2%/ o C (crystals) 0.5%/ o C (tubes) Longitudinal crystal uniformity Radiation damage Causes (?):