15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov GEANT EMCAL geometry for ALICE current status Aleksei Pavlinov WSU.

Slides:



Advertisements
Similar presentations
1 ALICE EMCal Electronics Outline: PHOS Electronics review Design Specifications –Why PHOS readout is suitable –Necessary differences from PHOS Shaping.
Advertisements

NLC – The Next Linear Collider Project Colorado Univ. - Boulder Calorimetry Cornell-ALCPG Calorimetry Detector Study Plans at Colorado Uriel Nauenberg.
NLC – The Next Linear Collider Project Colorado Univ. - Boulder Calorimetry-Arlington Calorimetry Detector Study Plans at Colorado Uriel Nauenberg for.
Quartz Plate Calorimeter Prototype Ugur Akgun The University of Iowa APS April 2006 Meeting Dallas, Texas.
DREAM Collaboration: Recent Results on Dual Readout Calorimetry. F.Lacava for the DREAM Collaboration Cagliari – Cosenza – Iowa State – Pavia – Pisa –
Jin Huang Los Alamos National Lab.  Cited from March collaboration Meeting EC group Internal Communication Jin Huang 2 Preshower ID power drop significantly.
SoLID EC Design for IHEP 2012/10. Basic Features of Preliminary Design Based on COMPASS Shashlyk module design. 0.5mm lead/0.12mm air gap/1.5mm scintillator/0.12mm.
W. Clarida, HCAL Meeting, Fermilab Oct. 06 Quartz Plate Calorimeter Prototype Geant4 Simulation Progress W. Clarida The University of Iowa.
30 March Global Mice Particle Identification Steve Kahn 30 March 2004 Mice Collaboration Meeting.
ALICE EMCal Physics and Functional Requirements Overview.
M.Gallinaro, ``Innovative Particle and Radiation Detectors’’, Siena, October slide 1 The CDF MiniPlug Calorimeter Forward Physics Conceptual.
1/9/2003 UTA-GEM Simulation Report Venkatesh Kaushik 1 Simulation Study of Digital Hadron Calorimeter Using GEM Venkatesh Kaushik* University of Texas.
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.
Proposal for IHEP participation in CBM ECAL
Geant4: Electromagnetic Processes 2 V.Ivanchenko, BINP & CERN
Status of EIC Calorimeter R&D at BNL EIC Detector R&D Committee Meeting January 13, 2014 S.Boose, J.Haggerty, E.Kistenev, E,Mannel, S.Stoll, C.Woody PHENIX.
The Design of Barrel Electromagnetic Calorimeter (BEMC) October Lu Jun-guang.
Study of response uniformity of LHCb ECAL Mikhail Prokudin, ITEP.
1 Speed up ALICE simulation with TFluka Ernesto Lopez Torres.
Jet/MET without JetMET meeting, 25-Oct-2001, S.Kunori1 Di-jet mass with LOSS = 2 vs 1 in CMSIM120 Shuichi Kunori U. of Maryland 25-Oct-2001 PRS: Physics.
Status of Projectile Spectator Detector A.Kurepin (Institute for Nuclear Research, Moscow) I. Introduction to PSD. II. Conception and design. III. Development.
Beam test results of Tile/fiber EM calorimeter and Simulator construction status 2005/03/05 Detector Niigata University ONO Hiroaki contents.
R&D on W-SciFi Calorimeters for EIC at Brookhaven E.Kistenev, S.Stoll, A.Sukhanov, C.Woody PHENIX Group E.Aschenauer and S.Fazio Spin and EIC Group Physics.
Shower Containment and the Size of a Test Calorimeter Adam Para, September 6, 2006.
Study of Sampling Fractions Shin-Shan Yu, A P, Hans Wenzel, October 18, 2006.
The Tungsten-Scintillating Fiber Accordion Electromagnetic Calorimeter for the sPHENIX Detector Craig Woody, for the PHENIX Collaboration Physics Department,
E.Kistenev Large area Electromagnetic Calorimeter for ALICE What EMC can bring to ALICE Physics and engineering constrains One particular implementation.
CMS Calorimeter HB- HB+ HE- HE+ HF- HF+ HO-2 HO-1 HO0 HO+1 HO+2
1 Calorimeter in G4MICE Berkeley 10 Feb 2005 Rikard Sandström Geneva University.
EMCal in ALICE Norbert Novitzky 1. Outline How Electro-Magnetic Calorimeters works ? Physics motivation – What can we measure with Emcal ? – Advantages.
1 Lead glass simulations Eliane Epple, TU Munich Kirill Lapidus, INR Moscow Collaboration Meeting XXI March 2010 GSI.
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,
Apollo Go, NCU Taiwan BES III Luminosity Monitor Apollo Go National Central University, Taiwan September 16, 2002.
1 Performance of a Magnetised Scintillating Detector for a Neutrino Factory Scoping Study Meeting Rutherford Appleton Lab Tuesday 25 th April 2006 M. Ellis.
ECAL PID1 Particle identification in ECAL Yuri Kharlov, Alexander Artamonov IHEP, Protvino CBM collaboration meeting
CBM ECAL simulation status Prokudin Mikhail ITEP.
FSC Status and Plans Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group PANDA Russia workshop, ITEP 27 April 2010.
first results from EMCal test beam
5-9 June 2006Erika Garutti - CALOR CALICE scintillator HCAL commissioning experience and test beam program Erika Garutti On behalf of the CALICE.
1 Hadronic calorimeter simulation S.Itoh, T.Takeshita ( Shinshu Univ.) GLC calorimeter group Contents - Comparison between Scintillator and Gas - Digital.
1 1 - To test the performance 2 - To optimise the detector 3 – To use the relevant variable Software and jet energy measurement On the importance to understand.
Calice Meeting Argonne Muon identification with the hadron calorimeter Nicola D’Ascenzo.
SPHENIX EMCAL R&D Craig Woody BNL sPHENIX Design Study Meeting September 7, 2011.
1 Diodes (APDs) for the Electromagnetic Calorimeter in the ALICE experiment Paola La Rocca University and INFN Catania Characterization of Avalanche Photo.
Geant4 Tutorial, Oct28 th 2003V. Daniel Elvira Geant4 Simulation of the CMS 2002 Hcal Test Beam V. Daniel Elvira Geant4 Tutorial.
FT Prototype Test Purpose: test the prototype of the FT Calorimeter and Scintillator Hodoscope Technique: prototype is installed under the Hall B photon.
Adam Para, Fermilab, February 16, Who Cares? What is the Problem? 2 Dual Readout Total Absorption calorimeter has very good energy resolution.
Edouard Kistenev for the PHENIX Collaboration Calorimetry based upgrade to PHENIX at RHIC CALOR 2012 Santa Fe, NM, June 4-8, 2012.
1 Plannar Active Absorber Calorimeter Adam Para, Niki Saoulidou, Hans Wenzel, Shin-Shan Yu Fermialb Tianchi Zhao University of Washington ACFA Meeting.
Gamma Detector of Plastic Scintillator Oct. 2, 2009 IP-BSM Group 1.
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.
Simulation studies of total absorption calorimeter Development of heavy crystals for scintillation and cherenkov readout Dual readout in the 4 th concept.
W Prototype Simulations Linear Collider Physics & Detector Meeting December 15, 2009 Christian Grefe CERN, Bonn University.
NLC – The Next Linear Collider Project Colorado Univ. - Boulder Calorimetry-Arlington Calorimetry Detector Study Plans at Colorado Uriel Nauenberg for.
Simulation and reconstruction of CLAS12 Electromagnetic Calorimeter in GSIM12 S. Stepanyan (JLAB), N. Dashyan (YerPhI) CLAS12 Detector workshop, February.
The Transition Radiation Detector for the PAMELA Experiment
CALICE scintillator HCAL
Hadronic Shower Structure in WHCAL Prototype
IHEP group Shashlyk activity towards TDR
Jet reconstruction in ALICE using the EMCal
CERN SPS and PS Tests 2007 Goals: Show we have a working EMCal system
State-of-the-art in Hadronic Calorimetry for the Lepton Collider
Testbeam comparisons arXiv:
Detector Configuration for Simulation (i)
Dual-Readout Calorimeter: DREAM
Reports for highly granular hadron calorimeter using software compensation techniques Bing Liu SJTU February 25, 2019.
BESIII TOF Digitization
Electron PID & trigger using EMCal
Presentation transcript:

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov GEANT EMCAL geometry for ALICE current status Aleksei Pavlinov WSU

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov Deposited energy – response of calorimeter Shower evolution  Light collection in Sc plates  Light attenuation in fibers  Quantum efficiency  Threshold and noise in the readout system 

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov TRD1  TRD2 : common structure TRD1 TRD2

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov TRD1  TRD2 :  response uniformity (only EMCAL)

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov TRD1  TRD2 :  response uniformity(complete ALICE) 1.In both cases response changes significantly around super module crack. 2. TRD1 case is more uniform inside super module than TRD2 one.

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov Radiation length distribution before EMCAL

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov TRD1  TRD2 : jet response uniformity(only EMCAL) 1. Calorimeter response is uniform for TRD2 case. 2. Non uniformity is around ~10-12% for case of TRD1 TRD1 is our choice

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov What changed in calorimeter design and Geant geometry? Calorimeter coverage: 60 0 <  <180 0  80 0 <  <110 0 Structure of GEANT geometry was changed – super modules are not the same Added gap between super module in phi directions – 1cm Sampling of calorimeter prototype is 1.6mm*1.6mm (sampling was 2mm*2mm in our simulation) Passive scintillator tile was added in front of module. Geant cuts (cutele and cutgam) were changed Sc: ILOSS=2 – continuous energy loss without generaion of  - rays and full Vavilov-Landau-Gauss fluctuation; cutele=1 MeV, cutgam=80KeV; PB: ILOSS=1(3) – continuous energy loss with generaion of  - rays and restricted Landau fluctuation; cutele=1 MeV, cutgam=80KeV;

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov EMCAL response vs Geant cuts(sampling) cutele=100kev cutgam=80kev 1.6mm*1.6mm cutele=1Mev cutgam=80kev

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov EMCAL response vs Geant cuts – 2 cutele=cutgam Old:  GeV CPU:  100 kev  0.85 sec/ev  default  50 kev  1.15 sec/ev  10 kev  11.2 sec/ev TRD1_2x2_FINAL_100DEG_10KEV

15-16 Oct 2005 Alice-USA meetingAleksei Pavlinov What to do for DOE review? 1.Commit to cvs last changing in EMCAL software and test 2.Make list for needing simulation and run it (big job) 3.Recalculate the sampling fraction coefficient (several days) 4.Recalculate hadronic response of EMCAL (big job) 5.Make needing physics analysis   0 /  separation  e/hadrons separation  jet reconstruction  ……