Charm production at STAR

Slides:



Advertisements
Similar presentations
Heavy flavor production in STAR. What can charm and beauty tell us about matter in heavy ion collisions? Manuel Calderón de la Barca Sánchez UC Davis for.
Advertisements

Mass, Quark-number, Energy Dependence of v 2 and v 4 in Relativistic Nucleus- Nucleus Collisions Yan Lu University of Science and Technology of China Many.
Heavy flavor flow from electron measurements at RHIC Shingo Sakai (Univ. of California, Los Angeles)
Aug , 2005, XXXV ISMD, Czech X.Dong, USTC 1 Open charm production at RHIC Xin Dong University of Science and Technology of China - USTC  Introduction.
417 th WE-Heraeus-Seminar Characterization of the Quark Gluon Plasma with Heavy Quarks Physikzentrum Bad Honnef June 25-28, 2008 Ralf Averbeck, Heavy-Flavor.
Heavy Flavor Physics in HIC with STAR Heavy Flavor Tracker Yifei Zhang (for the STAR HFT Group) Hirschegg 2010, Austria Outline:  Physics motivation 
Fukutaro Kajihara (CNS, University of Tokyo) for the PHENIX Collaboration Heavy Quark Measurements by Weak-Decayed Electrons at RHIC-PHENIX.
ISMD’05, Kromeriz, Aug 09  15, Heavy  Flavor (c,b) Collectivity – Light  Flavor (u,d,s) Thermalization at RHIC Kai Schweda, University of Heidelberg.
Charm & bottom RHIC Shingo Sakai Univ. of California, Los Angeles 1.
K*(892) Resonance Production in Au+Au and Cu+Cu Collisions at  s NN = 200 GeV & 62.4 GeV Motivation Analysis and Results Summary 1 Sadhana Dash Institute.
Probing Properties of the QCD Medium via Heavy Quark Induced Hadron Correlations Huan Zhong Huang Department of Physics and Astronomy University of California.
Bingchu Huang, USTC/BNL 1 Bingchu Huang (for STAR Collaboration) University of Science and Technology of China (USTC) Brookhaven National Laboratory (BNL)
03/14/2006WWND2006 at La Jolla1 Identified baryon and meson spectra at intermediate and high p T in 200 GeV Au+Au Collisions Outline: Motivation Intermediate.
Cold Nuclear Matter Effects on Open Heavy Flavor at RHIC J. Matthew Durham for the PHENIX Collaboration Stony Brook University
4/1/2010MRPC workshop at USTC, Lijuan Ruan (BNL)1 STAR di-lepton measurements Outline: Motivation and Introduction Results from 200 GeV p+p collisions.
Non-photonic electron production in STAR A. G. Knospe Yale University 9 April 2008.
SQM2006, 03/27/2006Haibin Zhang1 Heavy Flavor Measurements at STAR Haibin Zhang Brookhaven National Laboratory for the STAR Collaboration.
Jaroslav Bielčík Czech Technical University Prague High-p T physics at LHC, March 2008, Tokaj Open heavy flavor at RHIC.
Sourav Tarafdar Banaras Hindu University For the PHENIX Collaboration Hard Probes 2012 Measurement of electrons from Heavy Quarks at PHENIX.
Recent measurements of open heavy flavor production by PHENIX Irakli Garishvili, Lawrence Livermore National Laboratory PHENIX collaboration  Heavy quarks.
HFT + TOF: Heavy Flavor Physics Yifei Zhang University of Science & Technology of China Lawrence Berkeley National Lab TOF Workshop, Hangzhou, April,
PHENIX Heavy-Flavor Results Matt Snowball (LANL) on behalf of the PHENIX collaboration Hard Probes 2015.
Single Electron Measurements at RHIC-PHENIX T. Hachiya Hiroshima University For the PHENIX Collaboration.
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.
STAR Indiana University Manuel Calderón de la Barca Sánchez Indiana University STAR Collaboration Open Charm Production IN STAR Open Charm Production IN.
Aug. 4-9, 2005, QM2005, Budapest X.Dong, USTC 1 Open charm production at RHIC Xin Dong University of Science and Technology of China - USTC.
Open heavy flavor in STAR David Tlusty NPI ASCR, CTU Prague for the STAR collaboration STAR.
Open charm hadron production via hadronic decays at STAR
Heavy flavor production at RHIC Yonsei Univ. Y. Kwon.
1 STAR Open Heavy Flavor Measurements Gang Wang (UCLA) 1  Motivation  D 0 / D s / D*  Non-photonic electron  Summary.
Recent Charm Measurements through Hadronic Decay Channels with STAR at RHIC in 200 GeV Cu+Cu Collisions Stephen Baumgart for the STAR Collaboration, Yale.
Manuel Calderón de la Barca Sánchez UC Davis STAR Collaboration Hard Probes 2012 Cagliari, Sardinia, Italy. 30/May/2012.
Measurement of D-meson azimuthal anisotropy in Au+Au 200GeV collisions at RHIC Michael R. Lomnitz Kent State University Lawrence Berkeley National Laboratory.
Ralf Averbeck Stony Brook University Hot Quarks 2004 Taos, New Mexico, July 19-24, 2004 for the Collaboration Open Heavy Flavor Measurements with PHENIX.
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.
Probing the properties of dense partonic matter at RHIC Y. Akiba (RIKEN) for 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.
Ralf Averbeck, Stony Brook University XXXX th Rencontres de Moriond La Thuile, Italy, March 12-19, 2005 The Charm (and Beauty) of RHIC l Heavy flavor in.
JPS/DNPY. Akiba Single Electron Spectra from Au+Au collisions at RHIC Y. Akiba (KEK) for PHENIX Collaboration.
1 Guannan Xie Nuclear Modification Factor of D 0 Mesons in Au+Au Collisions at √s NN = 200 GeV Lawrence Berkeley National Laboratory University of Science.
1 Measurement of Heavy Quark production at RHIC-PHENIX Yuhei Morino CNS, University of Tokyo.
Strange Probes of QCD Matter Huan Zhong Huang Department of Physics and Astronomy University of California Los Angeles, CA Oct 6-10, 2008; SQM2008.
Outline Motivation The STAR/EMC detector Analysis procedure Results Final remarks.
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.
Jaroslav Bielčík for STAR collaboration Czech Technical University & NPI ASCR Prague 34-th International Conference on High Energy Physics 2008 Philadelphia,
Di-electron elliptic flow in
Outline Introduction LHC and ALICE Heavy-quark production in pp
The Heavy Flavor Tracker (HFT)
Recontres de Moriond, March
Hard Probes and Heavy Flavor from STAR
Heavy-flavor particle correlations - From RHIC to LHC
Jets as a probe of the Quark Gluon Plasma
Strange Probes of QCD Matter
Heavy-Flavour Physics in Heavy-Ion Collisions
ALICE and the Little Bang
Experimental Studies of Quark Gluon Plasma at RHIC
RAA predictions show enhancement highly sensitive to jet quenching
Status and Implications of PID measurements at high pT
Heavy Ion Physics in RUN14-16
Modification of Fragmentation Function in Strong Interacting Medium
Motivation for Studying Heavy Quarks
Performance of the STAR Heavy Flavor Tracker in measuring the charged B meson through B  J/Ψ + X decay Elizabeth Brost Department of Physics, Grinnell.
Strangeness in Quark Matter 2007
Scaling Properties of Identified Hadron Transverse Momentum Spectra
20th International Conference on Nucleus Nucleus Collisions
Single  production at forward rapidity by PHENIX
Measurement of charm and bottom production in RHIC-PHENIX
Shingo Sakai for PHENIX Collaborations (Univ. of Tsukuba)
Heavy-quark and Quarkonia production in high-energy heavy-ion collisions André Mischke 1st International Workshop on Multiple Partonic Interactions at.
Presentation transcript:

Charm production at STAR Yifei Zhang University of Science & Technology of China 10th Particle Physics Conference April 26-28, Nanjing, China Thanks to the conference organizers

Introductions Signal/Spectra Flow & energy loss Correlations Outline Introductions Signal/Spectra Flow & energy loss Correlations Summary & Outlook November 29, 2018 Yifei Zhang USTC

Why measure charm? Mb  4.8 GeV >> Tc, LQCD, Muds Mc  1.3 GeV Higgs mass: electro-weak symmetry breaking. (current quark mass) QCD mass: Chiral symmetry breaking. (constituent quark mass) Heavy quark masses are not modified by QCD vacuum. Strong interactions do not affect them. Important tool for studying properties of the hot-dense matter created at RHIC energy. Muller nucl-th/0404015 November 29, 2018 Yifei Zhang USTC

Charm production cross-section Charm quarks are believed to be mainly produced at early stage by initial gluon fusions. Sensitive to initial parton distribution function. Nuclear and medium properties at initial stage. Precondition for light flavor thermalization if charm flow.. Essential for recombination calculations of J/ production. M. Gyulassy & Z. Lin, PRC 51 (1995) 2177 Npart L.Yan, P.Zhuang, N.Xu PRL 97 (2006) 232301 PHENIX data nucl-ex/0611020 November 29, 2018 Yifei Zhang USTC

Relativistic Heavy Ion Collider (RHIC) Brookhaven National Laboratory (BNL), Upton, NY November 29, 2018 Yifei Zhang USTC

Charm measurements at STAR STAR measurements: Signal/Spectra D0  K c   + X (y=0, low pT) c  e + X Flow & energy loss Radial flow from NPE RAA from NPE Correlations e-h, e-D0 November 29, 2018 Yifei Zhang USTC

Charm measurement at STAR Direct D0 reconstruction muon from charm semileptonic decay electron from heavy quark semileptonic decay - semileptonic decay hadronic decay c  e+ + anything (B.R.: 10.3%) c  + + anything (B.R.: 8.2%) c  l+ + anything (B.R.: 9.6%) D0  K, B.R.: 3.83% November 29, 2018 Yifei Zhang USTC

Introductions Signal/Spectra Flow & energy loss Correlations Outline Introductions Signal/Spectra Flow & energy loss Correlations Summary & Outlook November 29, 2018 Yifei Zhang USTC

Direct D-meson reconstructions at STAR Phys. Rev. Lett. 94 (2005) STAR Preliminary A. Shabetai QM08 K invariant mass distribution in d+Au, Au+Au minbias, Cu+Cu minbias at 200 GeV collisions. November 29, 2018 Yifei Zhang USTC

D0 & Lepton from HF decay at STAR STAR Preliminary New Cu+Cu D0 spectrum agree with Au+Au after number of binary scaled. Low pT muon constrains charm cross-section. November 29, 2018 Yifei Zhang USTC

Charm cross-section Total cross-section with large theoretical uncertainty. d+Au: PRL 94 (2005) Cu+Cu: A. Shabetai QM08 Au+Au: Y. Zhang, JPG 32 (2006) S529 Both STAR and PHENIX are self-consistent. STAR results ~ 2 times larger than PHENIX Consistent with NLO calculation. November 29, 2018 Yifei Zhang USTC

Introductions Signal/Spectra Flow & energy loss Correlations Outline Introductions Signal/Spectra Flow & energy loss Correlations Summary & Outlook November 29, 2018 Yifei Zhang USTC

Radial flow – lepton from HF decays D0 STAR Preliminary STAR Preliminary Tfo = 220 MeV (best fit) – freeze out ealier <t> = 0.23 (best fit), <0.42 (1-). favor moderate or small radial flow. -- dense medium, light flavor thermalization. November 29, 2018 Yifei Zhang USTC

Charm energy loss, unsolved puzzle No direct D-meson measurement at high pT. Heavy flavor electron suppression was observed in several experiments. STAR PRL, 98, 192301 (2007) Radiative + Collisional eloss calculations describe data better. Question: Partonic eloss mechanism? Bottom contribution? November 29, 2018 Yifei Zhang USTC

Introductions Signal/Spectra Flow & energy loss Correlations Outline Introductions Signal/Spectra Flow & energy loss Correlations Summary & Outlook November 29, 2018 Yifei Zhang USTC

e-h correlations – conical emission Trigger on NPE from heavy quark decays. Section XIII: G. Wang Cu+Cu 200 GeV Au+Au 200 GeV STAR Preliminary Does heavy quark e-loss generate Mach Cone emission? November 29, 2018 Yifei Zhang USTC

e-h correlations – bottom contribution (be)/(ce+be) e-h: G. Wang, QM08 e-D0: A. Mischke, QM08 Simulation: ce, be, c+be Extract b/c ratio from the data/simulation comparison Good agreement among different analyses. Data consistent with FONLL. November 29, 2018 Yifei Zhang USTC

Does bottom affect charm X-sec? STAR Preliminary Before subtraction: (AuAu MB) (AuAu 0-12%) After bottom contribution subtraction: (AuAu MB) (AuAu 0-12%) Bottom contribution does NOT change charm cross-section (be)/(b+ce) upper limit of NLO is applied November 29, 2018 Yifei Zhang USTC

None zero charm flow is observed at RHIC energy. Summary Charm cross-section is found to follow number of binary collisions scaling. None zero charm flow is observed at RHIC energy. Electron suppression is observed at RHIC but the energy loss mechanism is still NOT really understood. Abounding correlations related to heavy flavor are reported. November 29, 2018 Yifei Zhang USTC

Outlook Currently… W/o inner tracker, direct measurement of D-mesons through topology reconstruction is impossible due to insufficient track projection resolution close to the collision vertex. Heavy Flavor Tracker Single muon can not be measured at high pT at STAR. Muon Telescope Detector Single electron is always suffered from the amount of photonic background. Full barrel Time Of Flight Detector Semileptonic decayed electron is not strongly sensitive to D-mesons. November 29, 2018 Yifei Zhang USTC