Directed Flow of Identified Particles

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Presentation transcript:

Directed Flow of Identified Particles Aihong Tang for the Collaboration Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010 A Few Useful Concepts x y z Reaction plane : Defined by the beam and the line connecting two colliding nuclei Transverse momentum : Peripheral collisions : collisions in which two nuclei barely graze each other. Central collisions : head-on collisions. Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

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 a convention to define the sign of v1 of spectators at forward rapidity as positive. Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

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 ISMD, Univ. of Antwerp, Belgium, Sept 2010

Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010 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 ISMD, Univ. of Antwerp, Belgium, Sept 2010

v1 and 1st order phase transition Central Peripheral dv1/dy at y=0 Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

v1 and early thermalization See next talk. Piotr Bozek, RHIC/AGS workshop 2010 Piotr Bozek and Iwona Wyskiel-Piekarska, Arxive:1009.0701 Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010 v1 at low energies 6 A GeV Au+Au e895, PRL 85 940 (2000) E895, PRL 86 2533 (2001) Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010 v1 at low energies peripheral mid-central central NA49, NPA 715, 583 (2003) Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

v1 at RHIC, measured by Phobos (= η-ybeam) Phobos, PRL 97 012301 (2006) Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

v1 at RHIC, measured by STAR STAR, PRL 101 252301 (2008) Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010 STAR Experiment EMC Barrel MRPC ToF Barrel EMC End Cap FMS BBC FPD TPC ZDC & ZDCSMD ZDC & ZDCSMD FTPC PMD Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

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 ISMD, Univ. of Antwerp, Belgium, Sept 2010

Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010 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 ISMD, Univ. of Antwerp, Belgium, Sept 2010

Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010 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 ISMD, Univ. of Antwerp, Belgium, Sept 2010

Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010 PID v1 at RHIC Preliminary Preliminary Difference seen between v1 of protons and anti-protons in 5-30% central collisions. Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

Centrality dependence of v1 slope 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. Considering antiproton/proton ratio is almost flat as a function of centrality, what is observed does not match expectations. Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010

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 ISMD, Univ. of Antwerp, Belgium, Sept 2010

Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010 Summary Negative slope of pions, antiprotons, protons and ks0 v1 is observed In mid-central collisions (5-30%), proton v1 slope becomes small (~-0.1%), and sizable difference is seen between v1 of protons and anti-protons. Anti-flow can explain the negative v1(y) slope but it has difficulties in explaining the centrality dependence of the difference between the v1(y) slope of protons and anti-protons. Aihong Tang ISMD, Univ. of Antwerp, Belgium, Sept 2010