Effect of Eccentricity Fluctuations on Elliptic Flow

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1 Effect of Eccentricity Effect of Eccentricity Fluctuations Fluctuations on Elliptic Flow on Elliptic Flow Art Poskanzer Color by Roberta Weir Exploring the secrets of the universe The Berkeley School 2010

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Effect of Eccentricity Fluctuations on Elliptic Flow. Exploring the secrets of the universe. Art Poskanzer. Color by Roberta Weir. The Berkeley School 2010. GSI-LBL Collaboration. July 1974 -- 36 years ago. Reinhard and Rudolf Bock walked into my office. Plastic Ball. Streamer Chamber. - PowerPoint PPT Presentation

Transcript of Effect of Eccentricity Fluctuations on Elliptic Flow

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Effect of Eccentricity FluctuationsEffect of Eccentricity Fluctuations on Elliptic Flow on Elliptic Flow

Effect of Eccentricity FluctuationsEffect of Eccentricity Fluctuations on Elliptic Flow on Elliptic Flow

Art PoskanzerColor by Roberta Weir

Exploring the secretsof the universe

The Berkeley School 2010

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GSI-LBL CollaborationGSI-LBL Collaboration

Reinhard and Rudolf Bock walked into my office

July 1974 -- 36 years ago

Plastic Ball Streamer Chamber

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Hermann GrunderHermann Grunder

2 Aug 74

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ReinhardReinhard

1976

1995

2001

Rudolf Bock1987

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2001

1996

1977

photo by Jef Poskanzer

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Filter theory to compare with dataFilter theory to compare with data

Plastic Ball, K.G.R. Doss et al., PRL 57, 302 (1986)

px/A

y/yproj

Directed Flow

transverse pin event plane

rapidity

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Best EllipsoidBest Ellipsoid

bounce

squeeze squeeze

Plastic Ball, H.H. Gutbrod et al., Phys. Lett. B216, 267 (1989)Diogene, M. Demoulins et al., Phys. Lett. B241, 476 (1990)Plastic Ball, H.H. Gutbrod et al., PRC 42, 640 (1991)

Negative elliptic flow

Squeeze-out

Q

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Analyze in the Transverse PlaneAnalyze in the Transverse Plane

P. Danielewicz and G. Odyniec, Phys. Lett. 157B, 146 (1985)

data mixed events

correlationof sub-eventplanes

Transverse Momentum Analysis

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Fourier HarmonicsFourier Harmonics

S. Voloshin and Y. Zhang, hep-ph/940782; Z. Phys. C 70, 665 (1996)

Fourier harmonics:

Event plane resolution correction made for each harmonic

See also, J.-Y. Ollitrault, arXiv nucl-ex/9711003 (1997)

Unfiltered theory can be compared to experiment!

and J.-Y. Ollitrault, Nucl. Phys. A590, 561c (1995)

Tremendous stimulus to theoreticians!

To remove acceptance correlations

Flatten event plane azimuthal distributions in lab

To measure event plane resolution

Correlate two independent sub-groups of particles

A.M. Poskanzer and S.A. Voloshin, PRC 58, 1671 (1998)

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Elliptic Flow vs. Beam EnergyElliptic Flow vs. Beam Energy

25% most centralmid-rapidity

all v2

six decades

In-planeelliptic flow

squeeze-out

bounce-offrotation

standard method

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Generating Function MethodsGenerating Function Methods

STAR, J. Adams et al., PRC 72, 014904 (2005)

CumulantsLee-Yang Zeros

Multi-particle methodseliminate 2-particle non-flowand Gaussian fluctuations

Minimize complex generating function to evaluate four-particle correlation

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Direct Four-Particle CorrelationDirect Four-Particle Correlation

Sergei Voloshin (2006)Dhevan Gangadharan, thesis, UCLA (2010)

4-particle correlations without a generating function

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v2{4} Direct Cumulantv2{4} Direct Cumulant

Dhevan Gangadharan, thesis, UCLA (2010)

acceptancecorrections

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Direct v2{4}Direct v2{4}

STAR preliminarySTAR preliminary

v2{2}

v2{4}Two independentimplementations agree

Sergei Voloshin, STARDhevan Gangadharan, STARNavnett Pruthi, STARAnte Bilandzic, ALICE

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MethodsMethods

“Two-particle”: v2{2}: each particle with every other particle

v2{subEP}: each particle with the EP of the other subevent

v2{EP} “standard”: each particle with the EP of all the others

v2{SP}: same, weighted with the length of the Q vector

Many-particle: v2{4}: 4-particle - 2 * (2-particle)2

Generating function or Direct Cumulant v2{q}: distribution of the length of the Q vector

v2{LYZ}: Lee-Yang Zeros multi-particle correlation

review of azimuthal anisotropy:arXiv: 0809.2949

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Integrated v2Integrated v2

STAR, J. Adams et al., PRC 72, 014904 (2005)

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MeasurementsMeasurements Two-particle methods

contain nonflow mean of some power of the distribution in the

Participant Plane

Multi-particle methods suppress nonflow mean in the Reaction Plane in Gaussian

approx.

Bhalerao and Ollitrault, Phys Lett. B 641, 260 (2006)Voloshin, Poskanzer, Tang, and Wang, Phys. Lett. B 659, 537 (2008)

nonflow

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Effect of Eccentricity Fluctuations on Elliptic Flow

Effect of Eccentricity Fluctuations on Elliptic Flow

Mean of some power of the distribution

Participant plane fluctuations

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root-mean-square

mean

full event

sub-event

Effect of Fluctuations on the MeanEffect of Fluctuations on the Mean

Ollitrault, Poskanzer, and Voloshin, PRC 80, 014904 (2009)Points: simulations by PHOBOS+

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Reaction, Participant, and Event PlanesReaction, Participant, and Event Planes

participant plane

coordinate space

momentum space

determined by impact parameter

determined by particles struck

Voloshin, Poskanzer, Tang, and Wang, Phys. Lett. B 659, 537 (2008)

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v2 Fluctuations from part Fluctuationsv2 Fluctuations from part Fluctuations

Assume width with same percent width as part:

is from standard deviation of nucleon MC Glauber of part

Bessel-Gaussian:

Voloshin, Poskanzer, Tang, and Wang, Phys. Lett. B 659, 537 (2008)

2D Gaussian fluctuationsin x and y in the reactionplane lead to Bessel-Gaussianfluctuations along theparticipant plane axis

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Theory is in RP, except...Theory is in RP, except... Event-by-Event without impact parameter

Kodama NeXSPheRIO Hydro for event-by-event participants

Hirano Determine PP for each event Rotate event to RP Thus include PP fluctuations in initial conditions

R. Andrade et al., Phys. Rev. Lett. 97, 202302 (2006)

T. Hirano and Y. Nara, PRC 79, 064904 (2009)

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EccentricitiesEccentricities

Hiroshi MasuiDrescher and Nara, PRC 76, 041903(R) (2007)

v2 driven by initial eccentricity

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Eccentricity FluctuationsEccentricity Fluctuations

Hiroshi MasuiDrescher and Nara, PRC 76, 041903(R) (2007)

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Assumptions

An Application to DataAn Application to Data

MC participant

less nonflow

Ollitrault, Poskanzer, and Voloshin, PRC 80, 014904 (2009)

Correct for nonflow

Correct to mean v2 in PP Correct to RP

nonflow

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agreement for mean v2

in participant plane

corrected to PP

Data Corrected to <v2>Data Corrected to <v2>published

Ollitrault, Poskanzer, and Voloshin, PRC 80, 014904 (2009)

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corrected to RP

v2 in the Reaction Planev2 in the Reaction Plane

in Gaussian fluctuation approximation:

Voloshin, Poskanzer, Tang, and Wang, Phys. Lett. B 659, 537 (2008)

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New ResultsNew Results

Direct Cumulants Non-Gaussian behavior

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Participant PlaneParticipant PlaneGlauber CGC

STAR preliminarySTAR preliminary

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Reaction PlaneReaction Plane

Glauber CGC

STAR preliminarySTAR preliminary

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Can Compare to TheoryCan Compare to Theory

Remove acceptance correlations Correct for Event Plane resolution Correct for mean of a power of the

distribution Correct for fluctuations of the PP

Because we now:

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dashed blue uses

Test Method Using part to stdTest Method Using part to std

Glauber

solid blue uses exact equations in Gaussian Model paper

Why does blue not godown to green?

Voloshin, Poskanzer, Tang, and Wang, Phys. Lett. B 659, 537 (2008)

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CGCCGC

Voloshin, Poskanzer, Tang, and Wang, Phys. Lett. B 659, 537 (2008)

CGC participant fluctuations lesspart and std much closer togetherso can say RP = std to more peripheral collisions

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Glauber part DistributionsGlauber part Distributions

Non-Gaussian for peripheral collisions

Gaussian and Bessel-Gaussian fits to the black calculations

Hiroshi Masui

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part < 1part < 1

can not be greater than 1

Hiroshi Masui

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StatusStatus Even though the eccentricity distribution

is not Gaussian, still could be:

However,

for peripheral collisions as estimated from Glauber calculations

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Emphasize Direct v2{4}Emphasize Direct v2{4} No Event Plane Corrects for acceptance correlations One pass through the data Eliminates 2-particle nonflow correlations Gives mean of the distribution Gives v2 in the RP

except for peripheral collisions