2000/9/23 JPS meeting in Niigata1 Measurement of single gamma and  0 with PHENIX EMCal (I) H.Torii Kyoto Univ./RIKEN for the PHENIX Collaboration. Sep/23/2000,

Slides:



Advertisements
Similar presentations
Multi-Particle Azimuthal Correlations at RHIC !! Roy A. Lacey USB - Chem (SUNY Stony Brook ) What do they tell us about Possible Quenching?
Advertisements

Photon-Jet Correlations at RHIC Saskia Mioduszewski Texas A&M University 18 July, 2007.
Measurement of charmonia at mid-rapidity at RHIC-PHENIX  c  J/   e + e -  in p+p collisions at √s=200GeV Susumu Oda CNS, University of Tokyo For.
09/30/'06SPIN2006, T. Horaguchi1 Measurement of the direct photon production in polarized proton-proton collisions at  s= 200GeV with PHENIX CNS, University.
10/03/'06 SPIN2006, T. Horaguchi 1 Measurement of the direct photon production in polarized proton-proton collisions at  s= 200GeV with PHENIX CNS, University.
1 Probing the medium with photons Outline: oMotivation oExperiment oResults oConclusion oIntroduction LBNL Saskia Mioduszewski Ahmed Hamed.
Recent Electroweak Results from the Tevatron Weak Interactions and Neutrinos Workshop Delphi, Greece, 6-11 June, 2005 Dhiman Chakraborty Northern Illinois.
Direct-Photon Production in PHENIX Oliver Zaudtke for the Collaboration Winter Workshop on Nuclear Dynamics 2006.
High p T  0 Production in p+p, Au+Au, and d+Au Stefan Bathe UC Riverside for the Collaboration Topics in Heavy Ion Collisions McGill University, Montreal,
A NLO Analysis on Fragility of Dihadron Tomography in High Energy AA Collisions I.Introduction II.Numerical analysis on single hadron and dihadron production.
W properties AT CDF J. E. Garcia INFN Pisa. Outline Corfu Summer Institute Corfu Summer Institute September 10 th 2 1.CDF detector 2.W cross section measurements.
Nov2,2001High P T Workshop, BNL Julia Velkovska High pt Hadrons from  sNN = 130 GeV Au-Au collisions measured in PHENIX Julia Velkovska (BNL) for PHENIX.
Physics Analysis with the PHENIX Electromagnetic Calorimeter Péter Tarján College of Nyíregyháza Zimányi 2009 Winter School on Heavy Ion Physics Budapest.
D 0 Measurement in Cu+Cu Collisions at √s=200GeV at STAR using the Silicon Inner Tracker (SVT+SSD) Sarah LaPointe Wayne State University For the STAR Collaboration.
Observation of W decay in 500GeV p+p collisions at RHIC Kensuke Okada for the PHENIX collaboration Lake Louise Winter Institute February 20, /20/20101.
Azimuthal anisotropy measurement of neutral pion and direct photon in  s NN =200GeV Au+Au collisions at RHIC-PHENIX TAC seminar 11/25/2008 Kentaro MIKI.
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.
Calibration of the PHENIX Lead Scintillator Calorimeter H.Torii for the PHENIX Collaboration Kyoto Univ./RIKEN Contents Lead Scintillator Calorimeter(PbSc)
Measurement of Inclusive Photon in Au+Au collisions by Conversion Method at RHIC-PHENIX T. Hachiya, Hiroshima Univ., for the PHENIX collaboration.
Measurement of J/  -> e + e - and  C -> J/  +   in dAu collisions at PHENIX/RHIC A. Lebedev, ISU 1 Fall 2003 DNP Meeting Alexandre Lebedev, Iowa State.
Measurements of thermal photons in heavy ion collisions with PHENIX - Torsten Dahms - Stony Brook University February 8 th, 2008 Real photons at low p.
M. Muniruzzaman University of California Riverside For PHENIX Collaboration Reconstruction of  Mesons in K + K - Channel for Au-Au Collisions at  s NN.
2004 Fall JPS meeting (English version) K.Okada1 Measurement of prompt photon in sqrt(s)=200GeV pp collisions Kensuke Okada (RIKEN-BNL research center)
Measurement of photons via conversion pairs with PHENIX at RHIC - Torsten Dahms - Stony Brook University HotQuarks 2006 – May 18, 2006.
27 Mar 2006 Kentaro MIKI for the PHENIX collaboration University of Tsukuba The Physical Society of Japan 61th Annual Meeting.
Charged Particle Multiplicity and Transverse Energy in √s nn = 130 GeV Au+Au Collisions Klaus Reygers University of Münster, Germany for the PHENIX Collaboration.
PHENIX Measurement of Parity-Violating Single Spin Asymmetry in W Production in p+p Collisions at 500 GeV Stephen Pate (for the PHENIX Collaboration) New.
Jet Physics at CDF Sally Seidel University of New Mexico APS’99 24 March 1999.
Bangalore, India1 Performance of GLD Detector Bangalore March 9 th -13 th, 2006 T.Yoshioka (ICEPP) on behalf of the.
Performance of the PHENIX Muon Identifier Introduction Calibration with cosmic rays Performance in Au+Au collisions Summary Hiroki Sato, Kyoto University.
Non-photonic electron production in p+p collisions at √s=200 GeV Xiaozhi Bai for the STAR collaboration Central China Normal University University of Illinois.
Nantes — 2008, July Analysis of results from EmCal beam test at CERN PS (and SPS) energies P. La Rocca & F. Riggi University & INFN Catania University.
JPS/DNPY. Akiba Single Electron Spectra from Au+Au collisions at RHIC Y. Akiba (KEK) for PHENIX Collaboration.
Study of J/  ->e + e - in d-Au Collision with Electron Triggers in PHENIX W. Xie (UC. Riverside) PHENIX Collaboration April APS in 2003.
Measurement of direct photon in \sqrt{s_NN}=200GeV Au+Au collisions at RHIC-PHENIX 東大 CNS Tadaaki Isobe for the PHENIX Collaboration Contents: 1.Motivation.
High Density Matter and Searches for Huan Z. Huang Department of Physics and Astronomy University of California, Los Angeles The STAR Collaboration.
24 Nov 2006 Kentaro MIKI University of Tsukuba “electron / photon flow” Elliptic flow measurement of direct photon in √s NN =200GeV Au+Au collisions at.
Hadronic resonance production in Pb+Pb collisions from the ALICE experiment Anders Knospe on behalf of the ALICE Collaboration The University of Texas.
High p T results from PHENIX Carla M Vale Brookhaven National Laboratory for the PHENIX Collaboration June
Mid-rapidity pi0 production in pp collisions at sqrt(s)=62 and 200 GeV measured by the PHENIX detector at RHIC A.Bazilevsky Brookhaven National Laboratory.
1 Prompt Photon Production from Proton - proton Collisions at √s = 62.4 GeV in PHENIX ( PHENIX 実験における重心系 62.4 GeV での陽子 - 陽子衝突からの 直接光子の生成断面積の測定 ) JPS meeting.
 -jet measurements Table of Contents:  Motivation  Preliminary QA of  -trigger Data  Shower Shape Analysis  Experimental Challenges  Summary  
Measurement of photons via conversion pairs with the PHENIX experiment at RHIC - Torsten Dahms - Master of Arts – Thesis Defense Stony Brook University.
11/23/2004 spin discussionK.Okada1 Measurement of prompt photon in  s=200GeV pp collisions Kensuke Okada For the PHENIX collaboration.
Toward a  +Jet Measurement in STAR Saskia Mioduszewski, for the STAR Collaboration Texas A&M University 1.
Brett Fadem of Muhlenberg College for the PHENIX Collaboration.
High p T hadron production and its quantitative constraint to model parameters Takao Sakaguchi Brookhaven National Laboratory For the PHENIX Collaboration.
Moriond 2001Jets at the TeVatron1 QCD: Approaching True Precision or, Latest Jet Results from the TeVatron Experimental Details SubJets and Event Quantities.
DE/dx in ATLAS TILECAL Els Koffeman Atlas/Nikhef Sources: PDG DRDC (1995) report RD34 collaboration CERN-PPE
Jan. 13, 2004Tomoaki Nakamura - Hiroshima Univ.1 Measurement of Fluctuations in Event-by-Event N ch -N γ Balance Tomoaki Nakamura and Kensuke Homma for.
9/11/2003Tomoaki Nakamura - Hiroshima Univ.1 Event-by-event charge/neutral fluctuation at RHIC-PHENIX Tomoaki Nakamura / Kensuke Homma Hiroshima University.
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.
Fall DNP Meeting,  meson production in Au-Au and d-Au collision at \ /s NN = 200 GeV Dipali Pal Vanderbilt University (for the PHENIX collaboration)
Azimuthal anisotropy measurement of direct photon in √s NN =200GeV Au+Au collisions at RHIC-PHENIX Photons should be emitted from several states such as.
Elena Bruna Yale University
“Performance test of a lead glass
High-pT Identified Hadron Production in Au+Au and Cu+Cu Collisions
The h double helicity asymmetry and cross section
Observation of Diffractively Produced W- and Z-Bosons
STAR Geometry and Detectors
RAA predictions show enhancement highly sensitive to jet quenching
First physics from the ALICE electromagnetic calorimeters
Simulation study for Forward Calorimeter in LHC-ALICE experiment
Kazuya Aoki For the PHENIX Collaborations. Kyoto Univ. / RIKEN
20th International Conference on Nucleus Nucleus Collisions
Jet Measurements with the EMCal of ALICE
High-pT Identified Charged Hadrons in √sNN = 200 GeV Au+Au Collisions
Observation of Diffractively Produced W- and Z-Bosons
Why 1 What 2 How 3 Measurement of Direct photon v2
Presentation transcript:

2000/9/23 JPS meeting in Niigata1 Measurement of single gamma and  0 with PHENIX EMCal (I) H.Torii Kyoto Univ./RIKEN for the PHENIX Collaboration. Sep/23/2000, JPS meeting in Niigata

2000/9/23 JPS meeting in Niigata2 Physics Motivation Quark Gluon Plasma(QGP) search –One of the hard probe for QGP is “Jet Quenching” –Jet Quenching. Quark energy loss in the QGP matter by gluon bremsstrahlung. Energy loss can be observed by measuring fragmented pi0 Xin-Nian Wang Phys.Rev.C (1998) Au+Au  s=200GeV (dE/dx=1GeV/c)

2000/9/23 JPS meeting in Niigata3 PbSc: Shish-Kebab sampling calorimeter PHENIX EM Calorimeter - PbSc (lead scintillator) and PbGl (lead glass) - Only Sector W0/W1 are used in this analysis. W1 W0 ~5m

2000/9/23 JPS meeting in Niigata4 Data Set & Event Selection Analyze Au+Au 130AGeV data sets –Only for PbSc parts. Sector W0/W1 –Aug/6 to Aug/18 Event Selection –[1126k events] $BBC Z vertex <  40cm –[419k events] $-2.5nsec<(ZDC T0 – BBC T0 – [ZDC T0-BBC T0] ) < 4.5nsec $BBC T0 < 13nsec –[371k events] cm Vertex Distribution Time 0 Distribution nsec RMS  3nsec

2000/9/23 JPS meeting in Niigata5 Geometrical Acceptance & Quality Assurance Check Geometrical Acceptance –Bottom 5 rows of W0 Sector are disabled <  < <  < (W0) <  <0.190 (W1) Quality Assurance Check –Disabled region 1.9 % Normal Position Acceptance W1 W0

2000/9/23 JPS meeting in Niigata6 TOF PID cut TOF width  1.4nsec –Still dominated by tower by tower calibration –Photon efficiency  100%(>1GeV) –Background contamination 50%-0% (Still large uncertainty in background contamination) Background contamination Photon efficiency Less background high E Large deviation from simulation at slower TOF.

2000/9/23 JPS meeting in Niigata7 Energy Calibration w/MIP First energy scale is calibrated by cosmic muon. 38MeV during construction Measured MIP energy in W0/W1 sectors. –June-July W0:  1.3MeV W1:  1.2MeV –Aug W0:  0.03MeV W1:  0.02MeV Gain shift during between June/July and Aug. –W0: 0.1  0.4% –W1: -7.0  0.4% Laser monitoring will be used soon in the analysis. Au+Au 130AGeV PHENIX Preliminary (Run ) Cosmic Muon

2000/9/23 JPS meeting in Niigata8 Energy Calibration w/  0 Energy Correction –Measured by PHENIX clustering algorithm PHENIX clustering algorithm is energy sum of a few core towers by considering shower profile. It’s to suppress overlapping effect Average energy obtained by PHENIX clustering algorithm is 93% of total shower. –Energy correction of MIP into 280MeV Correction is made for every 144 towers. Path length by geometrical effect is already accounted.  0 peak (Asymmetry 2.5GeV, TOF cut<2  ) –Before correction  1.9MeV –  =13.7  2.3MeV –After correction  1.8MeV –  =12.4  2.1MeV Absolute energy scale is roughly correct in 2% Invariant Mass after correction Invariant Mass before correction GeV

2000/9/23 JPS meeting in Niigata9 Table of Calibration Energy –Relative energy (every 144 towers)  2% (after <6% correction) –Absolute energy   2% (cosmic/hadron mip and pi0) –Time dependence  Studying by laser monitoring data TOF –Width  1.4nsec (mainly tower-by-tower calibration) Yield of photon –Geometrical acceptance  <  < <  < (W1) <  <0.190 (W0 ) –Quality assurance check  1.9% disabled –TOF PID photon efficiency/background contamination  efficiency>  100%, Background 50-0% (Still large uncertainty in background contamination) –Overlapping effect  Studying

2000/9/23 JPS meeting in Niigata10 EM Shower Energy Distribution Different total energy –TOF<2  –Normalized at 0.5GeV –No efficiency correction No TOF efficiency nor background contamination correction No shower overlapping effect correction –4 slopes seem to be similar –Is there any centrality dependence? Still Working on TOF efficiency/background contamination and overlapping effect Au+Au 130AGeV No efficiency corr. PHENIX Preliminary EM Shower Energy(GeV) Arbitrary GeV Total Energy

2000/9/23 JPS meeting in Niigata11 Summary PHENIX successfully completed first physics run from June to early- September in PHENIX EM calorimeter works and has measured signals. EM calorimeter calibration –Energy, TOF are calibrated by laser, MIP peak of cosmic  /charged hadron, an  0 mass Physics analysis is in progress. –EM shower energy distribution with different total energy. No Efficiency correction –TOF efficiency, background contamination are not corrected. –Shower overlapping effect is not corrected Slopes seem to be similar We still working on TOF efficiency/background contamination and overlapping effects. We will investigate centrality dependence