坂井 真吾 for the PHENIX Collaboration Shingo Sakai   Univ. of Tsukuba

Slides:



Advertisements
Similar presentations
Heavy flavor flow from electron measurements at RHIC Shingo Sakai (Univ. of California, Los Angeles)
Advertisements

Yorito Yamaguchi For the PHENIX collaboration CNS, University of Tokyo 10/14/2008ATHIC2008 1/13.
Measurement of elliptic flow of electrons from heavy flavor RHIC Shingo Sakai (Univ. of Tsukuba / JSPS)
Fukutaro Kajihara (CNS, University of Tokyo) for the PHENIX Collaboration Heavy Quark Measurements by Weak-Decayed Electrons at RHIC-PHENIX.
Charm & bottom RHIC Shingo Sakai Univ. of California, Los Angeles 1.
Di-electron Continuum at PHENIX Yorito Yamaguchi for the PHENIX collaboration CNS, University of Tokyo Rencontres de Moriond - QCD and High Energy Interactions.
Bingchu Huang, USTC/BNL 1 Bingchu Huang (for STAR Collaboration) University of Science and Technology of China (USTC) Brookhaven National Laboratory (BNL)
The Azimuthal Anisotropy of Electrons from Heavy Flavor Decays in √s NN =200 GeV Au-Au Collisions at PHENIX Shingo Sakai for PHENIX Collaborations (Univ.
Cold Nuclear Matter Effects on Open Heavy Flavor at RHIC J. Matthew Durham for the PHENIX Collaboration Stony Brook University
Sourav Tarafdar Banaras Hindu University For the PHENIX Collaboration Hard Probes 2012 Measurement of electrons from Heavy Quarks at PHENIX.
QM2006 Shanghai, China 1 High-p T Identified Hadron Production in Au+Au and Cu+Cu Collisions at RHIC-PHENIX Masahiro Konno (Univ. of Tsukuba) for the PHENIX.
QM’05 Budapest, HungaryHiroshi Masui (Univ. of Tsukuba) 1 Anisotropic Flow in  s NN = 200 GeV Cu+Cu and Au+Au collisions at RHIC - PHENIX Hiroshi Masui.
Single Electron Measurements at RHIC-PHENIX T. Hachiya Hiroshima University For the PHENIX Collaboration.
Heavy flavor production at RHIC Yonsei Univ. Y. Kwon.
RHIC – PHENIX 実験における単電子の測定 Single Electron Measurement at RHIC – PHENIX T. Hachiya Hiroshima Univ. For the PHENIX collaboration.
Electron and identified hadron v 2 to look for hadronic or partonic origin of elliptic flow Shingo Sakai for the PHENIX Collaboration Univ. of Tsukuba.
Energy Scan of Hadron (  0 ) Suppression and Flow in Au+Au Collisions at PHENIX Norbert Novitzky for PHENIX collaboration University of Jyväskylä, Finland.
Charm and J/PSI measurement at RHIC Y. Akiba (KEK) August 9, 2002 Riken Summer study 2002.
Measurement of Inclusive Photon in Au+Au collisions by Conversion Method at RHIC-PHENIX T. Hachiya, Hiroshima Univ., for the PHENIX collaboration.
Measurement of photons via conversion pairs with PHENIX at RHIC - Torsten Dahms - Stony Brook University HotQuarks 2006 – May 18, 2006.
Ralf Averbeck Stony Brook University Hot Quarks 2004 Taos, New Mexico, July 19-24, 2004 for the Collaboration Open Heavy Flavor Measurements with PHENIX.
1 Nuclear modification and elliptic flow measurements for  mesons at  s NN = 200 GeV d+Au and Au+Au collisions by PHENIX Dipali Pal for the PHENIX collaboration.
1 Fukutaro Kajihara (CNS, University of Tokyo) for the PHENIX Collaboration Heavy Quark Measurement by Single Electrons in the PHENIX Experiment.
Study of b quark contributions to non-photonic electron yields by azimuthal angular correlations between non-photonic electrons and hadrons Shingo Sakai.
JPS/DNPY. Akiba Single Electron Spectra from Au+Au collisions at RHIC Y. Akiba (KEK) for PHENIX Collaboration.
Feasibility study of Heavy Flavor tagging with charged kaons in Au-Au Collisions at √s=200 GeV triggered by High Transverse Momentum Electrons. E.Kistenev,
Heavy Flavor Workshop, Beijing, China, ShinIchi Esumi, Univ. of Tsukuba1 Heavy flavor collective flow measurements at RHIC ShinIchi Esumi Univ.
Elliptic flow of electrons from heavy flavor decays
1 Measurement of Heavy Quark production at RHIC-PHENIX Yuhei Morino CNS, University of Tokyo.
1 Measurements of Leptonic and Photonic Probes in Au+Au Collisions at PHENIX Run-2 Takashi Matsumoto for the PHENIX collaboration at RHIC & AGS Annual.
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.
Measurement of Azimuthal Anisotropy for High p T Charged Hadrons at RHIC-PHENIX The azimuthal anisotropy of particle production in non-central collisions.
Azimuthal Anisotropy and the QGP Yasuo MIAKE, Univ. of Tsukuba i)Why I Iike azimuthal anisotropy ii)Tsukuba strategy for RHIC-PHENIX iii)What is found.
Elliptic flow of electron from heavy flavor decay by the PHENIX Shingo Sakai for PHENIX collaboration (Univ. of Tsukuba & JPSP)
DNP/JPS 1 The azimuthal anisotropy of electrons from heavy flavor decays in √S NN = 200 GeV Au- Au collisions by PHENIX Shingo Sakai for the PHENIX collaborations.
Measurements of low pT direct photons in PHENIX Yorito Yamaguchi for the PHENIX collaboration CNS, University of Tokyo 04/11/2008WWND South Padre.
Direct Photon v 2 Study in 200 GeV AuAu Collisions at RHIC Guoji Lin (Yale) For STAR Collaboration RHIC & AGS Users’ Meeting, BNL, June 5-9.
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.
High-pT Identified Hadron Production in Au+Au and Cu+Cu Collisions
Maya SHIMOMURA University of Tsukuba for the PHENIX Collaboration
Takafumi Niida from Univ. of Tsukuba for the PHENIX Collaborations
Tatsuya Chujo for the PHENIX collaboration
Takafumi Niida from Univ. of Tsukuba for the PHENIX Collaborations
PHENIX measurement on direct photon production
Elliptic Flow in PHENIX
ShinIchi Esumi, Univ. of Tsukuba
Tatsuya Chujo University of Tsukuba (for the PHENIX Collaboration)
The Study of Elliptic Flow for PID Hadron at RHIC-PHENIX
Scaling Properties of Identified Hadron Transverse Momentum Spectra
20th International Conference on Nucleus Nucleus Collisions
Flow Measurement in PHENIX
Event anisotropy measurements in RHIC-PHENIX
High-pT Identified Charged Hadrons in √sNN = 200 GeV Au+Au Collisions
Hiroshi Masui for the PHENIX collaboration
Identified Charged Hadron
Search for the onset of baryon anomaly at RHIC-PHENIX
Shengli Huang Vanderbilt University for the PHENIX Collaboration
ShinIchi Esumi, Univ. of Tsukuba
Hiroshi Masui for the PHENIX collaboration August 5, 2005
Identified Charged Hadron Production at High pT
The azimuthal anisotropy in high energy heavy ion collisions at RHIC
Shingo Sakai for PHENIX Collaborations (Univ. of Tsukuba)
Shingo Sakai for PHENIX Collaborations (Univ. of Tsukuba)
ShinIchi Esumi, Univ. of Tsukuba
Systematic measurements of light vector mesons in RHIC-PHENIX
What have we learned from Anisotropic Flow at RHIC ?
Azimuthal anisotropy of electrons in Au+Au collisions at √SNN=200GeV/c measured with PHENIX at RHIC Shingo Sakai for PHENIX collaboration Univ. of Tsukuba.
Masahiro Konno (Univ. of Tsukuba) for the PHENIX Collaboration Contact
Hiroshi Masui For the PHENIX Collaboration Quark Matter 2004
Hiroshi Masui / Univ. of Tsukuba
Presentation transcript:

Elliptic flow of electrons/positrons in 200 GeV Au+Au collisions at RHIC-PHENIX 坂井 真吾 for the PHENIX Collaboration Shingo Sakai   Univ. of Tsukuba for the PHENIX Collaboration

Motivation(1) Clear excess about 1 GeV/c with respect Page 1 g conversion p0  gee h  gee, 3p0 w  ee, p0ee f  ee, hee r  ee h’  gee From Run1 result (PHENIX: PRL 88(2002)192303) Electron source Dalitz decays Di-electron decays Photon conversions Kaon decays Thermal dileptons charm decay beauty decay Inc.e/pho.e Electron sorce From Rnn1 resul Consiten Photonic Above 1 GeV/c charm decay contribution is large high pt electron v2 can carry information about the anisotropy of the parent charmed mesons PYTHIA Inc.e/pho.e High pt energy loss ? Clear excess about 1 GeV/c with respect to photon conversion and light hadron decay.

Motivation(2) The photonic-subtracted electron Page 2 direct g (J. Alam et al. PRC 63(2001)021901) b c The photonic-subtracted electron single spectra consistent with charm decay (binary scaled). “The high pt electron v2 can carry information about the anisotropy of the parent charmed mesons. “ PYTHIA Electron sorce From Rnn1 resul Consiten Photonic Above 1 GeV/c charm decay contribution is large high pt electron v2 can carry information about the anisotropy of the parent charmed mesons PYTHIA High pt energy loss ? photonic-subtracted electron

Measurement of v2e dN/d(-) = N (1 + 2v2obscos(2(-))) e - Page 3 <<Reaction Plane Method>> Measure azimuthal angle of each particle with respect to the reaction plane Y dN/d(-) = N (1 + 2v2obscos(2(-))) X Reaction Plane  : azimuthal angle of reaction plane : azimuthal angle of electrons v2obs: strength of azimuthal anisotropy (fitting of dn/d(-) or v2=<cos2(-)>) v2 = v2obs/ σ e - e r.p  wi*sin(2i) tan2  rp =  wi*cos(2i) σ=<cos(2(m-real))> = {<cos(2(A-B))>}1/2

Electron measurement at PHENIX Page 4 Electron measurement at PHENIX The PHENIX experiment has the unique capability to measure electrons at RHIC Electron identification : Cherenkov light in RICH - |h|  0.35 - pt 0.2~4.9 GeV/c Number of hit PMT Ring shape Geometry of PMT -installed North and South side of RHIC. -3 unit rapidity away from mad rapidity Electron identification

Reaction plane Determine r.p using BBC north and south Page 5 Correlation r.p BBC_north & r.p BBC_south r.p resolution <cos(2(A-real))> = {<cos(2(A-B))>}1/2 v2 =v2 obs / resolution Correlation r.p BBC_north & r.p BBC_south Centraryty Determine r.p using BBC central central peripheral Centrality [%]

dn/d distribution Page 6 v2e is corrected by subtracting miss ID of electrons e+(e-) candidate Miss ID e+(e-) -p/2 p/2 cand --- dn/dphi of candidate (detected RICH) e+(e-) miss ID --- dn/dphi of miss ID (dn/d)/N0 1.5 V2e is estimated by subtracting miss ID of electrons 1.0 1.0 dn/d of after subtract Miss ID e+(e-) 0.5 -p/2 p/2 pt 1.0 2.0 3.0 4.0

Pt dependence of v2(e) Page 7 v2 (M.B) pt[GeV/c] Systematic error R.P method (fitting / <cos2()>) electron ID V2e Simulation Photon conversion & Dalitz decay from pi0 It seem like that v2e originating from pi0 is not consistent with v2e which is including all electron sources Electron source Systematic error R.P method (fitting / <cos2()>) electron ID (M.B) pt[GeV/c]

Comparison with v2 of hadrons Page 8 v2 <<Low pt (pt<1.0GeV/c)>> v2(e) is larger than v2(pion)& v2 (proton) -> dominant pi0 decay - small decay angle - decay from higher pt v2 pion & v2 proton : nucl-ex/0305013 (PHENIX) v2 (proton) v2 (pion) v2(e) <<High pt (pt>2.0GeV/c)>> v2(e) seems like smaller than v2 (pion) Particular interest because of the contributions from heavy flavor (M.B) particular interest because of the contributions from heavy-quark (c/b) decays !(but the data include another sources now) (M.B) pt[GeV/c]

What is needed to estimate charmed electron v2 ? Page 9 What is needed to estimate charmed electron v2 ? Relative charm yield to the inclusive electron yield at Run2 (r= Np/Ne) electrons v2 originating photonic source Study v2 D->eX (due to large Q value) R=Nc/Ne

Summary Page10 Azumithal anisotropy of inclusive electrons/positrons are measured with respect to the reaction plane in 200 GeV Au+Au collision at RHIC-PHENIX. v2(e) is larger than v2 (pion) & v2 (proton) at low pt. v2(e) seems like smaller than v2 (pion) at high pt Next Run (Au+Au) will start soon. much more statistics (error bars will be much smaller)