PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration...

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PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute of Particle Physics, Wuhan, China

Transcript of PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration...

Page 1: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

PID v2 and v4 from Au+Au Collisions at √ sNN = 200 GeV at

RHIC

N. Li for the STAR Collaboration

Lawrence Berkeley National Laboratory, BerkeleyInstitute of Particle Physics, Wuhan, China

Page 2: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

Outline

2Na Li 25th Winter Workshop on Nuclear Dynamics

•Motivation•Analysis•Results•Summary

Page 3: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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Motivation

Formation of QGP in high-energynuclear collisions:

• De-confinement• Collectivity• Local thermalization

Important questions

We study with dataset of highest statistics

Page 4: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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Anisotropy Parametersspatial space

anisotropy

momentum space

anisotropy

1

2

3

3

cos),(21

dd

d

2

1

pd

d

nrTn

TT

nypv

ypp

NNE

rn nv cos

Azimuthal correlation with the reaction plane.

Built up in the early stage, therefore supplies the early information of matter generated in the collision.

Page 5: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

pQCD

ReCo & CoalescenceHydro

Motivation (cont.)

5Na Li 25th Winter Workshop on Nuclear Dynamics

Study the PID dependence of v2 and v4.

R. S. Bhalerao et.al PLB 627, 49; Borghini and Ollitrault, PLB 642, 227

Study Number-of-Quark scaling.

Range?

v4/v22 : a probe of ideal

hydro behavior.

STAR: Phys. Rev. C 77 (2008) 54901

Page 6: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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Anisotropy Parameter v2

Baryon and meson elliptic flow follow the number of quark ( Nq ) scaling.

Indicates that partonic flow builds up at RHIC.

STAR: Phys. Rev. C 77 (2008) 54901

How about the higher order anisotropic flow such as v4?

Page 7: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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Anisotropy Parameter v2 v4

Peter Kolb, PRC 68, 031902 STAR: Aihong Tang, Proc.24th Winter Workshop on Nuclear Dynamics

v4 : 4th harmonic

If system reaches local thermal equilibrium, according to ideal hydro dynamic calculation, v4/v2

2 approaches 0.5 at high pT region.

Directly related to the degree of thermalization of the medium.

Hydro, Boltzmann calculations: J. –Y. Ollitrault

Page 8: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

Dataset and Cuts

8Na Li 25th Winter Workshop on Nuclear Dynamics

Tracks used for TPC event plane:

No. of fit hits > 15

No. of fit hits/No. of possible hits >0.52

0.1 < pT < 2.0 GeV/c

| η | < 1.0

• System: Au+Au collision

• Energy : sNN = 200 GeV

• Event sample : ~60 M events• Year: 2007• Pseudorapidity range:

TPC : -1.0 < η < 1FTPC : -4.0 < η < -2.5 (east) 2.5 < η < 4.0 (west)

Tracks used for FTPC event plane:

6 =< No. of fit hits < 12

No. of fit hits/No. of possible hits > 0.52

0.1 < pT < 2.0 GeV/c

2.5< | η | < 4.0

Page 9: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

Event plane angle (Rad)

TPC Event Plane

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2nd harmonic event plane

Detector bias is removed by applying phi weights to the tracks.

Phi weights are generated by inverting the normalized phi distributions of detected tracks for a large event sample.

STAR preliminary (a)

STAR preliminary

(b)

(c)

Page 10: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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FTPC Event Plane1

' ( sin 2 cos 2 cos 2 sin 2 )n

n n n nn

J.Barrette et al. Phys. Rev. C56 (1997)3254

The event plane distribution is not flat after phi weight correction due to several acceptance effect of FTPC.

Add additional shift correction.

Large η gap is used to reduce the non-flow effect.

Phi weight + Shift

Phi weight

Event plane angle (Rad)

STAR preliminary

Page 11: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

Invariant Mass Method

11Na Li 25th Winter Workshop on Nuclear Dynamics

Borghini et al. Phys. Rev. C70 (2006)4905

2

2 2

( ) cos(2( )

( ) ( ) ( )

Sig Bginv r

Sig Bginv inv inv

v m

Sig Bgv m v m m

Sig Bg Sig Bg

Assume bmamv invinvBg )(2

KS0

STAR preliminary

STAR preliminary

Page 12: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

Pion and Proton Identification

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TPC: pi/K ~ 0.7 GeV/c pi+K/p ~1.1 GeV/c

pi/p ~ > 3GeV/c relativistic rise

Cuts used for identification:

No. of fit hits > 15

No. of fit hits/No. of possible hits >0.52

pT < 1 (GeV/c) -2 < nσπ (p) < 2pT > 2.5 (GeV/c) 0 < nσπ < 1 -1 < nσp < 0 M. Shao, et al., Nuclear Instruments

and Methods in Physics Research A 558 (2006) 419-429

pion purity: over 95% proton purity: 70%

The effect on proton v2 will be about 10%. )()(:

%70)(%30)(0

22

222

SKvKvAssume

pvKvv

Using Run 4 data result

Page 13: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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v2 {TPC} and v2 {FTPC}

v2(pT) have been measured for , p, KS0 and .

Non-flow effect reduced considerably by using the FTPC event plane.

STAR preliminary STAR preliminary

Au+Au 200GeV (minibias)

Page 14: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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Number of Quark (Nq) Scaling

STAR preliminary STAR preliminary

The number of quark scaling for , KS0 and holds

up to (mT – m)/nq ~ 1 GeV/c2.

Protons seem to deviate from the scaling at lower pT.

Page 15: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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v4 {TPC}

v4(pT) has been measured for , KS0 and .

The Nq scaling for v4 is observed at (mT - m)/nq < 1 GeV/c2, similar to that of v2.

STAR preliminary

STAR preliminary

Page 16: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

STAR preliminary

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Test of Ideal Hydro Predictions

v4 /v22 is about 1 at pT ~ 2 GeV/c, larger than the value

0.5 expected from ideal fluid calculations.

Page 17: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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Summary FTPC event plane is used in STAR in order to reduce the non-flow effect. Run 7 high statistics data used in this analysis.

Proton and anti-proton seems to deviate from the number of quark scaling at (mT - m)/nq ~ 1 GeV/c2 .

The number of quark scaling has been observed for v4 at (mT - m)/nq < 1 GeV/c2.

Mesons and baryons (, KS0 and ) have similar v4/(v2)2

ratios. It is close to unity at pT > 1 GeV/c, higher than ideal hydrodynamic model predictions.

Page 18: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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BACK UP

Page 19: PID v 2 and v 4 from Au+Au Collisions at √s NN = 200 GeV at RHIC N. Li for the STAR Collaboration Lawrence Berkeley National Laboratory, Berkeley Institute.

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Number of Quark (Nq) Scaling

STAR preliminary

STAR preliminary