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Hiroshi Masui / Univ. of Tsukuba for the Collaboration JPS, 62 nd Annual Meeting

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Measurement of Centrality dependence of identified hadron Elliptic Flow in  s NN = 200 GeV Au+Au collisions at RHIC - PHENIX. Hiroshi Masui / Univ. of Tsukuba for the Collaboration JPS, 62 nd Annual Meeting. Why Elliptic Flow ?. Z. Y. - PowerPoint PPT Presentation
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Hiroshi Masui / Univ. of Tsukuba JPS, Sep/24/2007 1/11 JPS, Sep/24/2007 Measurement of Centrality depe ndence of identified hadron Ellip tic Flow in s NN = 200 GeV Au+Au collisions at RHIC - PHENIX Hiroshi Masui / Univ. of Hiroshi Masui / Univ. of Tsukuba Tsukuba for the for the Collaboration Collaboration JPS, 62 JPS, 62 nd nd Annual Meeting Annual Meeting
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Page 1: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

1/11

JPS, Sep/24/2007

Measurement of Centrality dependence of identified hadron Elliptic Flow in sNN = 200 GeV Au+Au collisions at RHIC - PHENIX

Hiroshi Masui / Univ. of TsukubaHiroshi Masui / Univ. of Tsukuba

for the Collaborationfor the Collaboration

JPS, 62JPS, 62ndnd Annual Meeting Annual Meeting

Page 2: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

2/11Why Elliptic Flow ?• Sensitive probe in Sensitive probe in

the early stage of the early stage of heavy ion collisionheavy ion collisionss– Initial geometry overla

p (eccentricity)• Initial density + EOS• System size (number o

f collisions)

– Final momentum anisotropy (v2)

Rea

ctio

n pl

ane X

ZY

Px

Py Pz

Page 3: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

3/11Universal Scaling of v2 ?

• Universal scaling of vUniversal scaling of v22 suggest suggest– v2 for a variety of particle species

at RHIC are determined through (, KET/nq)

– Its magnitude is established in partonic level before hadronization

QM2006A. Taranenko

At mid-rapidity

Page 4: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

4/11Motivation

• Universal scaling of vUniversal scaling of v22 has been observed by has been observed by assumingassuming v2 of non-identified charged hadrons– v2 F(KET/nq)

• QuestionsQuestions– Are these assumptions really correct ?– The scaling of v2 is tested from central to mid-centr

al. How about peripheral collisions ?

• Study the validity of the scaling of vStudy the validity of the scaling of v22 in a wide in a wide range of centrality for identified hadronsrange of centrality for identified hadrons

Page 5: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

5/11PHENIX Experiment

• Vertex, CentralityVertex, Centrality– BBC, ZDC

• Event planeEvent plane– BBC (full azimuth, || = 3.0 - 3.9)

Large rapidity interval

• TrackingTracking– DC, PC

• PIDPID– TOF (||</4, ||<0.35), t ~ 120

ps , p : pT < 4 GeV/c, K : pT < 3 Ge

V/c

Page 6: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

6/11

• vv22 increase with increasing centrality increase with increasing centrality• Similar mass ordering for all centralitySimilar mass ordering for all centrality

Centrality dependence of v2(pT)

Page 7: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

7/11

• Scaling holds for all centrality ?Scaling holds for all centrality ?– Ratio of data to fit (next slide)

KET + NCQ scaling of v2

Page 8: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

8/11v2(Data)/v2(Fit)

• Scaling works within systematic errors, except for low KEScaling works within systematic errors, except for low KETT

– Radial flow ?

Page 9: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

9/11Eccentricity

• Eccentricity (Eccentricity () is e) is estimated by Glaubestimated by Glauber MC simulationr MC simulation value’s are not ch

anged so much in b = 5 - 9 fm (10 - 50 % centrality). / ~ 10 %

– Quite different for different definitions of at central and peripheral Systematic error on ~ 10 - 20 %

Page 10: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

10/11Eccentricity scaling• Scaled vScaled v22 with participa with participa

nt eccentricitynt eccentricity• Start to break even in Start to break even in

mid-central at high KEmid-central at high KETT

– Scaling works at low KET within systematic errors

• Clear difference betweClear difference between central and peripheren central and peripheralal– The difference of v2 is al

so observed for different eccentricity

* Only statistical errors are shown* Systematic error on ~ 10 - 20 %

Page 11: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

11/11Summary

• Study the scaling of vStudy the scaling of v22(p(pTT) for identified hadrons i) for identified hadrons in a wide range of centralityn a wide range of centrality

• KEKETT + quark number scaling + quark number scaling– Scaling holds within systematic errors, except for low

KET

– New RXNP detector could help us to • reduce systematic errors• add more statistics at peripheral events

• Eccentricity scalingEccentricity scaling– Scaling breaks even in mid-central at high KET

• works for low KET within systematic errors

– Clear difference between central and peripheral• Suggest that v2 v2 f(Npart)

Page 12: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

12/11Back up

Page 13: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

13/11Elliptic Flow at RHIC

• Substantial elliptic flow sSubstantial elliptic flow signals are observed for ignals are observed for a variety of particle speca variety of particle species at RHICies at RHIC

Page 14: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

14/11Event plane resolution

• Event plane resolution is determined by multiplicity and Event plane resolution is determined by multiplicity and vv22

– Maximum at mid-central• High multiplicity, small v2 at central• Low multiplicity, large v2 at peripheral

Page 15: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

15/11Terminology

• Definition of eccentricityDefinition of eccentricity std : Standard eccentricity var (participant eccentricity part) 2 (event plane eccentricity) : var, s

ubtract auto-correlation event-by-event (an idea from ShinIchi)

• WeightingWeighting part (coll)

• Calculated by weighting with Npart (Ncoll) distribution

• AveragingAveraging {2} 2

• Averaging of 2 over all events, then take square root

• More natural definition like measured v2

• Total : 3 Total : 3 2 2 2 = 12 definitions 2 = 12 definitions

Page 16: Hiroshi Masui / Univ. of Tsukuba for the                  Collaboration JPS, 62 nd  Annual Meeting

Hiroshi Masui / Univ. of TsukubaJPS, Sep/24/2007

16/11Eccentricity

• Estimated by Glauber MC simulationEstimated by Glauber MC simulation coll > part due to steeper Ncoll distributions compare

d to Npart


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