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High p T identified hadron anisotropic flow and Deuteron production in 200 GeV Au+Au Collisions. Shengli Huang Vanderbilt University for the PHENIX Collaboration. Outline:. Observables and Motivation Analysis methods Results and Discussion ,K,p(pbar) v 2 , v 4
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High pT identified hadron anisotropic flow and Deuteron production in 200 GeV Au+Au Collisions Shengli Huang Vanderbilt University for the PHENIX Collaboration
Outline: • Observables andMotivation • Analysis methods • Results and Discussion • ,K,p(pbar) v2, v4 • Deuteron production(dbar/d, RCP , B2…) • Conclusions S.L. Huang WWND08
reaction plane beam x y Anisotropic flow v2 and v4 Peter Kolb, PRC 68, 031902 momentum space asymmetry Spatial space asymmetry • Azimuthal correlation with the reaction plane • Built up in the early stage and self-quenched, therefore supply the early information of matter generated in the collision S.L. Huang WWND08
Partonic Flow PHENIX,PRL. 99, 052301 (2007) baryon meson • Baryon and meson elliptic flow follow the number of constituent quark scaling as a function of KET. This indicates that partonic flow builds up at RHIC • How about the higher order anisotropic flow such as v4? • Where is the break point where the hydro interfaces with jet fragmentation S.L. Huang WWND08
Star Preliminary V4/(v2)2 ratio • v4 /v22 is a probe of ideal • hydro behavior and related to • the degree of thermalization! • Peter Kolb, PRC 68, 031902 • R.S.Bhalerao et.al PLB 627,49; • Borghini and Ollitrault, PLB642,227 • Hydro dynamics predicts • v4 /v22 ~0.5 • The identified particles • v4/v22 ratio should provide more • detailed information than • that of charged hadron Y.T. Bai QM06 S.L. Huang WWND08
Recombination module • Large baryon/meson ratios, a factor of 3 above standard fragmentation • The data prefer to the particle production by the recombination in the intermediate pT • The deuteron will supply more information to check the recombination module S.L. Huang WWND08
PHENIX in Run 7 • Run 7: • ~5.5B events and around 50% have been used • A new Time of Flight detector (TOFw) has been installed in • the west arm of PHENIX • A new reaction plane detector (RxNP) has been installed in • the 38 cm < |z| < 42 cm alone the beam S.L. Huang WWND08
TOFw and Aerogel Detectors • TOFw intrinsic timing resolution is ~ 75ps • /K can be separated to 2.8 GeV/c , K/p can be separated • to 4.5 GeV/c and deuteron can be identified to 6~7GeV/c • 3. Together with Aerogel detector(ACC), we can identify the K to • pT~4 GeV/c and , p to 7 GeV/c S.L. Huang WWND08
Reaction plane Measurements • RxNP: • Two sets of plastic • scintillators positioned • on either side of the • collision vertex • 12 segments in • 2 segments in • 1.0 < || < 1.5 • 1.5 < || < 2.8 • BBC: • 3.1<||<3.9 • Both detectors are away from mid-rapidity. Smaller non-flow effect • on the reaction plane measurements • New RxNP detector resolution is around 74% at mid-centrality S.L. Huang WWND08
KET Scaling of v4 A.Taranenko • The mass ordering has also been observed for v4 • The number of constituent quark scaling holds for v4 when • KET/nq < 1 GeV. This confirms that matter with partonic degrees • of freedom has been generated at RHIC S.L. Huang WWND08
V4/(v2)2 ratio • The ratio of v4/(v2)2 is close to • 0.9 for the , K and p • Mesons and baryons have similar • v4/(v2)2 ratio What can we extract from this? S.L. Huang WWND08
Perfect Partonic Liquid Partons just in similar momentum space can recombine with each other Mesons and baryons have equal v4/(v2)2 Meson Baryon a) Perfect Partonic Liquid! L.W. Chen, C.M. Ko nucl-th 0602025 b) Partons in different momentum space also can recombine with each other S.L. Huang QM08
Charged v2 • Charged v2 can be measured to • 6 GeV/c. • The results are consistent with • 0 results in the overlap pT region. • All v2 start to drop at pT ~ 2.5 GeV/c • in the different centrality bins! S.L. Huang WWND08
Kaon and Proton v2 • Kaon v2 can be measured to 4 GeV/c and protons v2 can be measured to 6 GeV/c • Proton v2 starts to drop at pT ~ 4 GeV/c S.L. Huang WWND08
Break Point? KET/nq(GeV) KET/nq(GeV) • In the centrality of 20~60%, the , K and p KET scaling seemingly begins to • break at KET/nq ~ 1 GeV • More statistics are required for the further investigation S.L. Huang WWND08
Deuteron pTSpectra H. Valle QM08 The deuteron and anti-deuteron yield have been measured to pT~5 GeV/c in difference centrality S.L. Huang WWND08
dbar/d ratio vspT • Similar to pbar/p ratio, no pT and centrality dependence has been observed for the dbar/d ratio • The dbar/d ratio is 0.46±0.01(stat)±0.05(sys) and p/bar is 0.73 ± 0.01 • The dbar/d ratio is close to the (pbar/p)2 S.L. Huang WWND08
Deuterons Rcp The deuteron RCP peaks at pT~3~3.5GeV/c with the value around 2.8 S.L. Huang WWND08
Coalescence Parameter B2 pd = 2pp • The B2 of d and dbar as a function of pT in difference centrality • B2 increases from central to peripheral collisions • B2 rises with pT S.L. Huang WWND08
B2 and System Volume • Significant change in B2 from 14.5 to 60 Npart • 1/B2 vs Npart shows a consistent linear rise S.L. Huang WWND08
Centrality dependence of Source size Phys.Rev.Lett.93, 152302 (2004) • Radii shows linear increase as the cubic root of the number of participants (Npart) • Consistent with HBT radii for pions. S.L. Huang WWND08
Conclusions New time of flight detector(TOFw) of PHENIX runs successfully in Run 7 with 75 ps intrinsic timing resolution. With new TOFw, we have measured the identified charged hadrons v2 to pT~6 GeV/c, v4 to 4GeV/c and deuteron spectra to 5GeV/c The number of constituent quark scaling has been observed for v4 for KET/nq < 1 GeV. Mesons and bayrons have similar v4/(v2)2 ratio which is close to 0.9 The number of constituent quark scaling seemingly begins to break for v2 as KET/nq~1GeV at 20~60% centrality The d/dbar ratio has no pT and centrality dependence and the deuteron Rcp peaks at pT~3~3.5GeV/c with the value around 2.8 The coalescence parameter (B2) and source radius extracted from deuteron production indicate that the source radius decreases with pT but increases linearly with Npart1/3, which is consistent with expanding source S.L. Huang WWND08