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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba1 Heavy flavor collective flow measurements at RHIC ShinIchi Esumi Univ. of Tsukuba In collaboration with : H. Huang, Y. Miake, S. Sakai, N. Xu, Y. Zhang
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba2 x z Non-central Collisions locally thermal Radial Collective Expansion Analysis of Collectivity in Heavy Ion Collisions Radial Flow Elliptic and Directed Flow boost coalescence/hydro jet suppression/geometry
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba3 PHENIX preliminary annihilation compton scattering Bremsstrahlung (energy loss) prompt photon v 2 = 0 v 2 < 0 thermal photon v 2 > 0 Jet-frag. photon from the survived parton v 2 > 0 direct photon as a probe of bulk matter consistent with prompt photon production, but we are free to speculate. QM06
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba4 STAR preliminary v 2 scaling with m T -m + number of quark v2v2 p T (GeV/c) RQMD Au+Au 200GeV Feng Liu, QM06 No separation in freeze-out Mass effect after freeze-out Feed down effect masked Low p T part squeezed Scaling in RQMD mass m T slope A+A p+p radial flow QM06
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba5 N e : inclusive electron yield material amounts : 0 1.1% 1.7% Dalitz : 0.8% X 0 equivalent 0 With converter Conversion in converter W/O converter 0.8% Non-photonic Conversion from known material ? % Photonic cocktail method converter method eID with RICH B.G. BG subtracted energy – momentum matching Method
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba6 Non-photonic electron spectra and R AA nucl-ex/0611018
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba7 Non-photonic electron R AA vs p T (centrality dependence) QM06
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba8 π v 2 nucl-ex/0608033 Estimation of photonic electron v 2 simulation subtraction
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba9 v 2 incl. = N non-ph. v 2 non-ph. + N phot. v 2 phot. N non-ph. + N phot. Non-photonic electron v 2 QM06
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba10 centrality dependence of non-photonic electron v2 compared with hadrons PHENIX RUN2 PHENIX RUN4
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba11 hint #0 of charm quark collectivity STAR nucl-ex/0611018
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba12 u/d/(s) quarks v2 c quark v2 quark p T (GeV/c) quark v 2 Shingo preliminary D meson v 2 p T (GeV/c) PHENIX preliminary data electron v 2 from D meson decay v2 D (p T ) ~ v2 q (p T *1/6) + v2 c (p T *5/6) Estimation of D-meson and charm quark v 2 (I) SQM06 v 2 shape assumption for D-meson magnitude fitted to minimize 2
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba13 minimum result D->e 22 44 11 2 minimum : a = 1, b = 0.96 ( 2 /ndf = 22/27) v 2 (u,d,s) ~ v 2 (c) universal v 2 (p T ) for quark v2 (p T ) ~ 2*v2 q (p T *1/2) v2 p (p T ) ~ 3*v2 q (p T *1/3) v2 D (p T ) ~ v2 q (p T *1/6) + v2 q (p T *5/6) Simultaneous fitting of /K/p/e v 2 Estimation of D-meson and charm quark v 2 (II) QM06
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba14 Does it follow the scaling with other hadrons? This is when we assume D meson v2 has same pT dependence as proton. This is at the lower limit of D meson v2 from the previous page 12. We can not rule out that D-meson flowing with other hadrons. Quark mass difference is neglected here. (n q =2) QM06
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba15 HP06 Estimation of B-meson contribution
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba16 HP06 combination of D- and B-meson We need to increase B contribution further more even with v 2b =0. It will be more difficult to explain R AA.
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba17 HP06 D meson only (b/c=0) case : no-bottom at all Charm v 2 reduction at high p T is preferred. electron v 2 from D-meson alone with v 2 reduction at high p T
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba18 Pythia D-meson decay electron p T D-meson p T case 1 case 2 input D-meson v2 output electron v2 input D-meson v2 output electron v2 1 st 2 nd 3 rd 4 th 5 th iteration Difference between expected and output electron v 2 is used to feed back the input D- meson v 2 without shape assumption. Slight difference in feed back procedure and expected electron v2 between case1 and case2.
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba19 case 1 case 2 electron v 2 from D-meson alone without assumption in D-meson v 2 shape input pythia D-meson v2 output pythia electron v2 expected electron v2 (parameterized by experimental data) v2v2 p T (GeV/c)
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba20 AuAu Central charm hadron AuAu Central , K, p AuAu Central strangeness hadron SQM06, Yifei Zhang hint #1 of charm quark collectivity
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba21 N. Xu, SQM 2006, PHENIX ( , K, p, J/ ): PRC69, 034909(04), QM05; STAR ( , , ): QM05 RHIC SPS hint #2 of charm quark collectivity PHENIX J/ PBM et. al. QM06
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba22 hint #3 of charm quark collectivity QM06
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba23 heavy flavor tracker, silicon vertex detector direct measurement D meson v 2 new reaction plane detector good resolution => reduce error from R.P. J/ψ v 2 & high pT non-photonic electron v 2 Reaction plane detector for PHENIX Heavy Flavor Tracker for STAR Vertex Tracker, Forward Calorimeter for PHENIX
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Heavy Flavor Workshop, Beijing, China, 2006.11.22ShinIchi Esumi, Univ. of Tsukuba24 Summary Charm quark shows collectivity at RHIC.
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