Collective Flow Measurements from the PHENIX Experiment

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Collective Flow Measurements from the PHENIX Experiment ShinIchi Esumi for the PHENIX Collaboration CONTENTS higher order event anisotropy event plane correlation v 2 ,v 3 ,v 4 in 200GeV Au+Au 2-particle correlation energy dependence of v n direct-photon v 2. y. - PowerPoint PPT Presentation

Transcript of Collective Flow Measurements from the PHENIX Experiment

  • Collective Flow Measurements from the PHENIX Experiment ShinIchi Esumi for the PHENIX Collaboration

    CONTENTShigher order event anisotropyevent plane correlationv2,v3,v4 in 200GeV Au+Au2-particle correlationenergy dependence of vndirect-photon v2

    ShinIchi Esumi, Univ. of Tsukuba

  • zyxReaction Plane (x-z)yxyxarXiv:1003.0194v3 and Initial Fluctuationblack-disk --> sign-flipping v3 initial fluctuation --> no-sign-flipping v3

    ShinIchi Esumi, Univ. of Tsukuba

  • BBCMPCPbW04 2cm Pb converter in frontRXN(zero degree n calorimeterZDC/SMD /shower max detector)(reaction plane detector)(muon piston EM-calorimeter)(beam-beam quartz-Cherenkov detector)05-5dN/dCNT(PHENIX central tracking arm)Wide range of coverage with several R.P. detectors for systematic studies

    ShinIchi Esumi, Univ. of Tsukuba

  • centrality (%)n=2 RXNn=3 RXNn=4 RXNn=2 MPCn=3 MPCn = positive correlation in 3 between opposite up to 3 ~ 4Reaction plane resolution of nth order planeRXN || = 1.0 ~ 2.8 MPC || = 3.1~ 3.7 200GeV Au+AuPHENIX Preliminarybetter resolutionNo sign flipping in 3 observed--> Initial geometrical fluctuation

    ShinIchi Esumi, Univ. of Tsukuba

  • same harmonics 2(2-2) ~ 10% 3(3-3) ~ 1%

    weak negative correlation between 3 and 1

    hint for rapidity anti-symmetric v3 contribution

    No visible correlation between 3 and 2arXiv:1105.3928A: RXN(>0)B: BBC(0)D: MPC(

  • arXiv:1105.3928charged particle vn : ||
  • v3 provides an additional constraining power on the hydro-model. Glauber & 4/s=1 works CGC-KLN & 4/s=2 failsv3 breaks the degeneracyv2v3arXiv:1105.3928B. Alver et. al., Phys. Rev. C82, 034913(2010).B. Schenke et. al., Phys. Rev. Lett. 106, 042301(2011).H. Petersen et. al., Phys. Rev. C82, 041901(2010).GlauberCGCSmaller eccentricity Larger eccentricity Glauber & 4/s=1 favored

    ShinIchi Esumi, Univ. of Tsukuba

  • Identified /K/p v3{3} at 200GeV Au+Aucommon systematic error for all 3 specieslower pT particle mass dependence radial flow

    intermediate pT baryon / meson splitting quark coalescence at hadronization with partonic v3 Radial & Partonic collective flow seen in v3

    ShinIchi Esumi, Univ. of Tsukuba

  • Df(rad)DhRidgeMach-ConeDoes v3 explain Ridge and Mach-Cone?Ridge : long range correlation at near-side Cone : double peak/shoulder at away-side (long in )v3 : initial fluctuation is common over wide range of

    ShinIchi Esumi, Univ. of Tsukuba

  • (CNT)(RXN)C2()data - fit + 1clear 3rd order moment seen in long range correlation

    another way of extracting the vn parameters with forward anisotropy vn without using nCNTRXN2-particle correlation between central and forward200GeV Au+Au 20~30%PHENIX PreliminaryRXN: ||=1.0~2.8CNT: (||

  • 2-particle correlation between central and centralB. Alver et. al., Phys. Rev. C82, 034913(2010).Bulk flow + jet(cent.-cent. 2-part.)Bulk flow(forw. 3 E.P.)v3Hydro model with Glauber & 4/s=1workssmall difference

    ShinIchi Esumi, Univ. of Tsukuba

  • Flow subtraction/correction with measured vn for central-central 2-particle correlationv2 ,v3 ,v4 BG corrected

    PHENIX preliminary200GeV Au+Au0-20%, inc. g-had.v2 BG correctedmach-cone is mostly goneremaining medium effect seen(correlated pair yield by absolute normalization)

    ShinIchi Esumi, Univ. of Tsukuba

  • 2 R.P.penetration dominancesurface dominance2 R.P.Trig.Trig.Trig.Trig.Trigger angle selected 2-part. corr. data are plotted in polar coordinate by rotating 2 R.P. angle as X-axis. Observed left/right asymmetry remains after the usual/normal v3 subtraction.in-plane trigger caseout-of-plane trigger caseFlow subtracted yield is shown radially with base line.200GeV Au+Au -> h-h (pTTrig=2~4, pTAsso=1~2GeV/c)v2(v4{2})-only subtractionPHENIX preliminaryTwo competing processes seenTrigger angle selection w.r.t. 2 separately for left(up) / right(down)

    ShinIchi Esumi, Univ. of Tsukuba

  • v2{2}, v3{3}, v4{4} at 62GeV Au+Aucharged particle vn : ||
  • Beam energy dependence 39/62/200GeV Au+Au2-particle correlation method between central and forward rapiditiessimilar hydro-properties down to 39GeVcharged particle v3charged particle v2charged particle v4

    ShinIchi Esumi, Univ. of Tsukuba

  • Identified hadron v2 at 39GeV Au+AuPHENIX PreliminaryPHENIX PreliminaryPartonic collective flow down to 39GeV(similar for 62GeV Au+Au)

    ShinIchi Esumi, Univ. of Tsukuba

  • Comparable v2 vs pT from 39GeV to 2.76TeVALICE Experiment, PRL105,252302 (2010)similar hydro-properties from 39GeV to 2.76TeV

    ShinIchi Esumi, Univ. of Tsukuba

  • Preliminary, STAR, PHENIX and E895 dataSaturation of v2 with beam energysaturation of v2 for given pT around or below 39GeV

    still increases mainly because of the rise.103104ALICEAlmost perfect fluidity from 39GeV to 2.76TeVat 1.7GeV/cat 0.7GeV/c

    ShinIchi Esumi, Univ. of Tsukuba

  • Measurement of 0 and inc. v2200GeV Au+Au (min. bias)arXiv:1105.4126significant difference between 0 and inc. v2 above 5GeV/c, difference between v2{RXN} and v2{BBC} due to jet bias.

    ShinIchi Esumi, Univ. of Tsukuba

  • R ratio and extracted dir. v2200GeV Au+Au (min. bias)arXiv:1105.4126dir. v2 is small at high pT --> consistent with prompt photon surprisingly large dir. v2 seen, similar to hadron v2 at low pT.

    ShinIchi Esumi, Univ. of Tsukuba

  • pT (GeV/c)dir. v2Large v2 of low pT thermal photon --> challenge to theory calculationsComparison of dir. v2 with model calculations200GeV Au+Au 0-20%R. Chatterjee and D. K. SrivastavaPRC 79, 021901(R) (2009)PRL96, 202302 (2006)Several models have failed in v2 magnitude with similar shape

    ShinIchi Esumi, Univ. of Tsukuba

  • ShinIchi Esumi, Univ. of Tsukuba

  • Related PHENIX talks

    PHENIX Measurements of Higher-order Flow Harmonics in Au+Au Collisions at sqrt(s_NN)=200 GeV: Implications for Initial-eccentricity Models and the Specific Viscosity of the Quark Gluon Plasma [Mon.23-May-2011 18:30-18:50 Parallel 1-7 Global and collective dynamics]Roy Lacey (Stony Brook Phys.) Measurement of Light Vector Mesons by PHENIX Experiment at RHIC[Mon.23-May-2011 18:50 Parallel 1-8 Hadron thermodynamics and chemistry]Deepali Sharma (Weizmann)

    Probing Nuclear Matter With Jets and gamma-Hadron Correlations:Results from PHENIX [Tues.24-May-2011 17:00 Parallel 2-1 Jets]Nathan Grau (Columbia)

    Identified particle v3 measurements at 200GeV Au+Au collisions at RHIC-PHENIX experiment[Mon.24-May-2011 17:20-19:30 Poster Session 1 + Wine and cheese]Sanshiro Mizuno (Univ. of Tsukuba)

    Measurements of low mass dielectrons in Au+Au collisionswith the HBD upgrade of the PHENIX detector[Thur.26-May-2011 16:00 Parallel 5-3 Electromagnetic probes]Mihael Makek (Weizmann)

    Direct photon production in heavy ion collisions in PHENIX experiment at RHIC [Thur.26-May-2011 16:40 Parallel 5-3 Electromagnetic probes]Edouard Kistenev (BNL Phys.)

    Collision energy dependence of the flow and spectra results in Au+Au collisions at sqrt(s_NN)=7.7-200 GeV from PHENIX [Fri.27-May-2011 17:50-18:10 Parallel 5-4 Global and collective dynamics] Xiaoyang Gong (Stony Brook Chem.)

    ShinIchi Esumi, Univ. of Tsukuba

  • Summary and Outlook

    Significant higher order event anisotropy observedConsistent with initial geometrical fluctuationBreak degeneracy: Glauber & 4/s=1 favoredStrong impact on Mach cone and ridge

    Almost perfect fluidity from 39GeV to 2.76TeV

    Direct photon v2 observedSmall at high pT --> consistent with pQCD Large in low pT --> challenge to theory

    ShinIchi Esumi, Univ. of Tsukuba

  • Backup slides

    ShinIchi Esumi, Univ. of Tsukuba

  • Event plane resolution and raw tracknR.P. distribution PHENIX Preliminaryestimated from RXN(S) - RXN(N) || = 1~2.8 = 2 MPC(S) - MPC(N) || = 3.1~3.7 = 6.22 , 3 and 4 are defined for each event. 200GeV Au+Au

    ShinIchi Esumi, Univ. of Tsukuba

  • A: RXN(N,>0)B: BBC(S,0)D: MPC(S,
  • Correlation between different harmonics (w.r.t spectator 1ZDC)centrality (%)A: BBC(S) [-3.9,-3.1] B: BBC(N) [3.1,3.9] sin term sin term

    (%)C: ZDC(S+N) |5 1 (1 - 1ZDC(S+N))2 (2 - 1ZDC(S+N))3 (3 - 1ZDC(S+N))200GeV Au+AuPHENIX Preliminaryclear sign-flipping in v1 , clear positive v2indication of sign-flipping in v3 , sign(v1) = sign(v3)(N-side flipped to combine)0001060.06(%)(%)200GeV Au+AuPHENIX Preliminary200GeV Au+AuPHENIX Preliminary

    ShinIchi Esumi, Univ. of Tsukuba

  • ShinIchi Esumi, Univ. of Tsukuba

  • comparison with theory calculations at 200GeV Au+AuarXiv:1105.NNNNHydro-models succeed with Glauber initial fluctuation. 200GeV Au+Aucharged particle vn

    ShinIchi Esumi, Univ. of Tsukuba

  • v2 v3PHENIX preliminarywith central-central2-particle-correlationat ||>0.32-particle correlation within central arm ||
  • vn

    pT=2-2.5GeV/c pT=0.75-1GeV/cen : nth order glauber geom. anisotropy0.5 x enNpart

    ShinIchi Esumi, Univ. of Tsukuba

  • v2{2}, v3{3}, v4{4} at 39GeV Au+Aucharged particle vn : ||
  • vnvn

    ShinIchi Esumi, Univ. of Tsukuba

  • PHENIX preliminaryPHENIX preliminary

    ShinIchi Esumi, Univ. of Tsukuba

  • ShinIchi Esumi, Univ. of Tsukuba

  • Method of event plane determination

    (1) Detector calibration / cell-by-cell calibration(2) Q-vector, re-centering, normalization of width Q{n}x = i { wi cos (n i) } Q{n}x = (Q{n}x - ) / Q{n}x Q{n}y = i { wi sin (n i) } Q{n}y = (Q{n}y - ) / Q{n}y Q{1}xZDC = i { wi xi } / i { wi } Q{1}yZDC = i { wi yi } / i { wi }(3) n-th harmonics reaction plane{n} = atan2 (Q{n}y , Q{n}x) / n(4) Fourier flattening (Sergeis+Arts method paper) n {n} = n {n} + i (2/i) { - cos(i n {n}) + sin(i n {n}) }(5) measure vn w.r.t. n and correct for E.P. resolution

    2-particle correlation among 3-sub detectors ForwardHit (F), BackwardHit (B), CentralTrack (C)

    (1) measure d distribution between 2 detectors weighting by the hit amplitude (2) normalize by the event mixing to make correlation functions for 3 combinations(3) fit the correlation with Fourier function to extract vnFvnB, vnFvnC and vnBvnC(4) vnF(Hit) and vnB(Hit) can be determined as a function of centrality(5) vnC(Track) can be determined as a function of centrality and pT

    ShinIchi Esumi, Univ. of Tsukuba

  • PRL104 (2010) 062301 Some couplings betweenmach-cone-like and ridge-like emissions and v3 are expected to be there!

    What is the origin and what is the consequence?ridge shoulder

    ShinIchi Esumi, Univ. of Tsukuba

  • n-even :vn() = vn(-)

    n-odd :vn() = -vn(-)all n :vn() = vn(-)case1case2case3

    ShinIchi Esumi, Univ. of Tsukuba

  • 200GeV Au+Au 20~30%PHENIX Preliminary

    CNT: central tracksmid-rapidity (||

  • central-central 2-part. correlation with Dh dependence0
  • flow subtraction with measured vn for cent-cent 2-par. correlation200GeV Au+Au0-20%, inc. g-had.Fourier spectra of extracted jet shape

    ShinIchi Esumi, Univ. of Tsukuba

  • ASSO-TRIG0thick side mach-cone (shoulder region)ASSO-TRIG
  • Flow subtracted 2-particle correlation with trigger angle selection in 200GeV Au+Au200GeV Au+Au -> h-h (pTTrig=2~4GeV/c, pTAsso=1~2GeV/c)v2(v4{2})-only subtraction PHENIX preliminaryout-of-planein-planeaverage0-20%20-50%50-93%

    ShinIchi Esumi, Univ. of Tsukuba

  • 12345678Jet , Trig.Jet , Trig.1234567856781234Jet , Trig.jet, di-jet and multi-particle correlation with various conditions

    ShinIchi Esumi, Univ. of Tsukuba

  • real photon v2 and external conversion photon v20-20%20-40%40-60%200GeV Au+Au

    ShinIchi Esumi, Univ. of Tsukuba

  • 0-20%20-40%40-60%200GeV Au+AuInclusive photon v2 and 0 v2

    ShinIchi Esumi, Univ. of Tsukuba

  • 0-20%20-40%40-60%200GeV Au+AuInclusive photon v2 and decay photon v2

    ShinIchi Esumi, Univ. of Tsukuba

  • 0-20%20-40%40-60%200GeV Au+Audirect photon v2

    ShinIchi Esumi, Univ. of Tsukuba

  • 0, inclusive, direct v2200GeV Au+Au (min. bias)arXiv:1105.NNNNsimilar to hadron v2 at low pTmuch smaller v2 at high pT

    ShinIchi Esumi, Univ. of Tsukuba

  • ShinIchi Esumi, Univ. of Tsukuba

  • ShinIchi Esumi, Univ. of Tsukuba

  • Holopainen, Rsnen, Eskola arXiv:1104.5371v1V. S. PantuevarXiv:1105.4033v1Au+Au 30-35%

    ShinIchi Esumi, Univ. of Tsukuba

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