Directed Flow Measurements at STAR

Slides:



Advertisements
Similar presentations
M. Oldenburg Theory Seminar, University of Frankfurt, January Directed Flow in Au+Au Collisions Markus D. Oldenburg Lawrence Berkeley National Laboratory.
Advertisements

M. Oldenburg Johann Wolfgang Goethe-Universität Frankfurt, Januar Gerichteter Fluss bei Au+Au Kollisionen (Directed Flow in Au+Au Collisions) Markus.
M. Oldenburg Probing QCD with High Energy Nuclear Collisions, Hirschegg, Austria, January Directed Flow in Au+Au Collisions Markus D. Oldenburg.
PID v2 and v4 from Au+Au Collisions at √sNN = 200 GeV at RHIC
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.
STAR 1 Azimuthal Anisotropy: The Higher Harmonics Art Poskanzer for the Collaboration STAR.
Anisotropic Flow at RHIC Jiayun Chen (for Collaboration) Institute of Particle Physics, HZNU, Wuhan, , P.R.China Brookhaven National Lab, Upton,
Quark Matter 2006 ( ) Excitation functions of baryon anomaly and freeze-out properties at RHIC-PHENIX Tatsuya Chujo (University of Tsukuba) for.
Identified particle transverse momentum distributions in 200 GeV Au+Au collisions at RHIC 刘海东 中国科技大学.
System size and beam energy dependence of azimuthal anisotropy from PHENIX Michael Issah Vanderbilt University for the PHENIX Collaboration QM2008, Jaipur,
Identified and Inclusive Charged Hadron Spectra from PHENIX Carla M Vale Iowa State University for the PHENIX Collaboration WWND, March
High p T identified hadron anisotropic flow and Deuteron production in 200 GeV Au+Au Collisions Shengli Huang Vanderbilt University for the PHENIX Collaboration.
High p T identified charged hadron v 2 and v 4 in 200GeV AuAu collisions by the PHENIX experiment Shengli Huang Vanderbilt University for the PHENIX Collaboration.
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.
1 Identified particle production in the Beam Energy Scan from STAR Anthony Timmins for the STAR Collaboration  The Beam energy scan  The STAR experiment.
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.
Partonic Collectivity at RHIC ShuSu Shi for the STAR collaboration Lawrence Berkeley National Laboratory Central China Normal University.
1 2-particle correlation at RHIC Fabrice Retière, LBNL for the STAR collaboration.
20 Nov 2006, Quark Matter, Shanghai, ChinaShinIchi Esumi, Univ. of Tsukuba1 Rapporteur 3 Bulk Properties and Collective Phenomena ShinIchi Esumi Univ.
Soft Physics at RHIC Michal Šumbera Nuclear Physics Institute AS CR, Řež/Prague (for the STAR and PHENIX Collaborations) 1 Hadron Collider Physics Symposium.
Energy Dependence of ϕ -meson Production and Elliptic Flow in Au+Au Collisions at STAR Md. Nasim (for the STAR collaboration) NISER, Bhubaneswar, India.
LP. Csernai, NWE'2001, Bergen1 Part II Relativistic Hydrodynamics For Modeling Ultra-Relativistic Heavy Ion Reactions.
1 Low energy scan and collective flow at 9 GeV Jiayun Chen, Feng Liu, Shusu Shi, Kejun Wu Weihai, Aug. 9,2009.
Incident-energy and system-size dependence of directed flow Gang Wang (UCLA) for STAR Collaboration  Introduction to directed flow  Detectors: ZDC-SMD,
Hadron Collider Physics 2012, 12/Nov/2012, KyotoShinIchi Esumi, Univ. of Tsukuba1 Heavy Ion results from RHIC-BNL ShinIchi Esumi Univ. of Tsukuba Contents.
Masashi Kaneta, First joint Meeting of the Nuclear Physics Divisions of APS and JPS 1 / Masashi Kaneta LBNL
Aihong Tang The Berkeley School 05 1 Open Questions in the “Perfect Fluid” Aihong Tang.
Beam-Energy and Centrality Dependence of Directed Flow of Identified Particles Prashanth Shanmuganathan (for the STAR Collaboration) Kent State University,
V 2 and v 4 centrality, p t and particle-type dependence in Au+Au collisions at RHIC Yuting Bai for the STAR Collaboration.
PHENIX. Motivation Collaboration PHENIX Roy A. Lacey (SUNY Stony Brook) PHENIX Collaboration I N T E R N A T I O N A L W O R K S H O P O N T H E P H.
Observation of antimatter hypernuclei at RHIC Jinhui Chen Kent State University for the STAR Collaboration 10 th International Conference on Hypernuclear.
Chiral Magnet Effect, where are we?
Directed flow of identified particles from Au+Au Collisions at RHIC
PHENIX Measurements of Azimuthal Anisotropy at RHIC
Directed Flow of Identified Particles
Directed flow of identified particles from Au+Au Collisions at RHIC
High-pT Identified Hadron Production in Au+Au and Cu+Cu Collisions
for STAR Collaboration
Strangeness Production in Heavy-Ion Collisions at STAR
Soft Physics at Forward Rapidity
Example analysis of toy model
Bulk Properties and Collective Phenomena
Collective Dynamics at RHIC
Anisotropic flow at RHIC: How unique is the NCQ scaling ?
Tatsuya Chujo for the PHENIX collaboration
Starting the Energy Scan - First Results from 62
Yields & elliptic flow of and in Au+Au collisions at
Tatsuya Chujo University of Tsukuba (for the PHENIX Collaboration)
The Study of Elliptic Flow for PID Hadron at RHIC-PHENIX
Outline Background Global Observables in Heavy Ion Collisions
Anisotropic flow at RHIC from SPS to RHIC
for the PHENIX collaboration
Scaling Properties of Identified Hadron Transverse Momentum Spectra
Institute of Particle Physics Huazhong Normal University
Anisotropic RHIC Hiroshi Masui / Univ. of Tsukuba Mar/03/2007 Heavy Ion Cafe.
Anisotropic flow at RHIC - selected topics
Flow Measurement in PHENIX
Energy dependence of stopping
High-pT Identified Charged Hadrons in √sNN = 200 GeV Au+Au Collisions
Hiroshi Masui for the PHENIX collaboration
Search for the onset of baryon anomaly at RHIC-PHENIX
Identified Charged Hadron Production
Shengli Huang Vanderbilt University for the PHENIX Collaboration
Hiroshi Masui for the PHENIX collaboration August 5, 2005
Identified Charged Hadron Production at High pT
Directed Flow from Au+Au Collisions at 200 GeV
What have we learned from Anisotropic Flow at RHIC ?
Masahiro Konno (Univ. of Tsukuba) for the PHENIX Collaboration Contact
Identified Particle Production at High Transverse Momentum at RHIC
Hiroshi Masui / Univ. of Tsukuba
Presentation transcript:

Directed Flow Measurements at STAR Aihong Tang for the Collaboration Aihong Tang Moriond QCD March 2011

A few useful concepts in heavy ion collisions x y z Reaction plane : Defined by the beam and the line connecting two colliding nuclei Peripheral collisions : collisions in which two nuclei barely graze each other. Central collisions : head-on collisions. Aihong Tang Moriond QCD March 2011

Definitions: directed flow (v1), elliptic flow (v2) X Z XZ – the reaction plane Picture: © UrQMD rapidity <px> or v1=<px/pt> x y z py px initial spatial anisotropy anisotropy in momentum space directed elliptic isotropic It is a convention to define the sign of v1 of spectators at forward rapidity as positive. Aihong Tang Moriond QCD March 2011

Anti-flow / 3rd flow component 8 A GeV flow antiflow Brachmann, Soff, Dumitru, Stocker, Maruhn, Greiner Bravina, Rischke , PRC 61 (2000) 024909. L.P. Csernai, D. Roehrich PLB 458, 454 (1999) M.Bleicher and H.Stocker, PLB 526,309(2002) Anti-flow/3rd flow component : Flat v1 at midrapidity due to 1st order phase transition Caution : Seeing anti-flow does not necessarily mean that there is a QGP EoS. (refer to UrQMD). In following slides, anti-flow only means zero or negative slope at midrapidity, due to the fast expansion of a tilted source. Aihong Tang Moriond QCD March 2011

Aihong Tang Moriond QCD March 2011 v1 from baryon stopping RQMD v2.4 AuAu 200 GeV R.Snellings, H.Sorge, S.Voloshin, F.Wang, N. Xu, PRL (84) 2803(2000) Baryon stopping + positive space-momentum correlation  v1 wiggle. No QGP necessary Aihong Tang Moriond QCD March 2011

v1 and early thermalization Piotr Bozek and Iwona Wyskiel-Piekarska, PRC 83, 024910 (2011) Sensitive to the tilt, the initial time (not shown) and the relaxation time. Aihong Tang Moriond QCD March 2011

Aihong Tang Moriond QCD March 2011 STAR Experiment EMC Barrel MRPC ToF Barrel EMC End Cap FMS BBC FPD TPC ZDC & ZDCSMD ZDC & ZDCSMD FTPC PMD Aihong Tang Moriond QCD March 2011

v1 at RHIC, viewed with η/ybeam Preliminary Clear patterns for spectators and “transported + produced” particles. Aihong Tang Moriond QCD March 2011

v1 at RHIC, viewed in η-ybeam Preliminary Phobos, PRL 97 012301 (2006) Similar if viewed in the projectile frame – Limiting Fragmentation Hypothesis (It remains as a hypothesis, unfortunately !) Aihong Tang Moriond QCD March 2011

v1 at RHIC, system size independence Piotr Bozek and Iwona Wyskiel-Piekarska, PRC 81, 054902 (2010) STAR, PRL 101 252301 (2008) AMPT failed to describe data. Hydro+”anti-flow” works (but failed in describing PID flow – see later). Aihong Tang Moriond QCD March 2011

Aihong Tang Moriond QCD March 2011 PID v1 at RHIC Preliminary Anti-proton slope has the same sign of pions – consistent with anti-flow Kaon suffers less shadowing effect due to smaller k/p cross section, yet we found negative v1 slope for Kshort – consistent with anti-flow Aihong Tang Moriond QCD March 2011

Aihong Tang Moriond QCD March 2011 PID v1 at RHIC AuAu 200 GeV Preliminary Preliminary Difference seen between v1 of protons and anti-protons in 5-30% central collisions. No difference is seen in “Hydro + anti-flow” model (not shown). Aihong Tang Moriond QCD March 2011

Centrality dependence of v1 slope AuAu 200 GeV Preliminary Negative v1 slope for protons is observed in 30-80% centralities. Large difference seen between v1 of protons and anti-protons in 5-30% centralities. Anti-flow alone cannot explain the data. Aihong Tang Moriond QCD March 2011

Proton v1 Excitation Function Preliminary 5-10% 4.2 +/-0.1(stat)+/-0.1(sys) fm 10-20% 5.9 +/-0.2(stat)+/-0.2(sys) fm 20-30% 7.6 +/- 0.2(stat)+/-0.2(sys) fm Rapidity window used in STAR : [-0.6,0.6] Proton v1 in mid-central collisions at RHIC stays small Aihong Tang Moriond QCD March 2011

Aihong Tang Moriond QCD March 2011 Summary Directed flow probes the early dynamics. Directed flow has been measured by STAR over a wide η/ybeam range at different energies. The directed flow is found to be independent of system size, and its value at forward region is confirmed to scale with η-ybeam for a wide energy range. Anti-flow alone cannot explain the difference in v1 between protons and anti-protons. So far no models can explain all features simultaneously. Aihong Tang Moriond QCD March 2011

Aihong Tang Moriond QCD March 2011 BackUp Aihong Tang Moriond QCD March 2011

Aihong Tang Moriond QCD March 2011 v1 at low energies 6 A GeV Au+Au e895, PRL 85 940 (2000) E895, PRL 86 2533 (2001) Aihong Tang Moriond QCD March 2011

Aihong Tang Moriond QCD March 2011 v1 at low energies peripheral mid-central central NA49, NPA 715, 583 (2003) Aihong Tang Moriond QCD March 2011

Data set for PID v1 analysis Run7 , 62 M events. Preliminary Preliminary Tracks used for TPC : No. of fit hits ∈[15, 50] Global DCA∈[0.0, 1.0] No. of fit hits/No.of possible hits ∈[0.52, 1.05] 0.1 < pT < 12.0 GeV/c | η | < 1. PID achieved by TPC dE/dx Pt cut for protons/anti-protons [0.4,1 GeV/c] Aihong Tang Moriond QCD March 2011

Aihong Tang Moriond QCD March 2011 Pion v1 at RHIC Au+Au 200GeV 10%-70% RQMD: Phys. Rev. Lett. 84 (2000) 2803; UrQMD: Phys. Lett. B 526 (2002) 309; AMPT: Phys. Rev. C 81, 014904 (2010); QGSM+ Partonic recombination: Phys. Rev . C 76 (2007) 024912; hydro + tilted source: Piotr Bo˙zek and Iwona Wyskiel, arXiv:1002.4999 [nucl-th] (2010). Preliminary Hydro+tilted source describes the data the best Aihong Tang Moriond QCD March 2011

v1 and 1st order phase transition Central Peripheral dv1/dy at y=0 Aihong Tang Moriond QCD March 2011