Effect of Eccentricity Fluctuations on Elliptic Flowrnc.lbl.gov/Poskanzer/TBS10.ppt.pdfElliptic Flow...
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Effect of Eccentricity FluctuationsEffect of Eccentricity Fluctuations on Elliptic Flow on Elliptic Flow
Art PoskanzerColor by Roberta W eir
Exploring the secretsof the universe
The Berkeley School 2010
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GSI-LBL Collaboration
Reinhard and Rudolf Bock walked into my office
July 1974 -- 36 years ago
Plastic Ball Streamer Chamber
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Hermann Grunder
2 Aug 74
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Reinhard
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 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 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 flowSqueeze-out
Q
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Analyze 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 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 correlationsFlatten event plane azimuthal distributions in lab
To measure event plane resolutionCorrelate two independent sub-groups of particles
A.M. Poskanzer and S.A. Voloshin, PRC 58, 1671 (1998)
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10A. Wetzler (2005)
Elliptic 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 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 Correlation
Sergei Voloshin (2006)Dhevan Gangadharan, thesis, UCLA (2010)
4-particle correlations without a generating function
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v2{4} Direct Cumulant
Dhevan Gangadharan, thesis, UCLA (2010)
acceptancecorrections
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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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Methods● “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 v2
STAR, J. Adams et al., PRC 72, 014904 (2005)
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Measurements● 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
● 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 Mean
Ollitrault, Poskanzer, and Voloshin, PRC 80, 014904 (2009)Points: simulations by PHOBOS+
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Reaction, 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 εpart Fluctuations
Assume width with same percent width as εpart:σε is from standard deviation of nucleon MC Glauber of εpart
Bessel-Gaussian:
Voloshin, Poskanzer, Tang, and Wang, Phys. Lett. B 659, 537 (2008)
2D Gaussian fluctuationsin εx and εy in the reactionplane lead to Bessel-Gaussianfluctuations along theparticipant plane axis
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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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Eccentricities
Hiroshi MasuiDrescher and Nara, PRC 76, 041903(R) (2007)
v2 driven by initial eccentricity
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Eccentricity Fluctuations
Hiroshi MasuiDrescher and Nara, PRC 76, 041903(R) (2007)
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● Assumptions
An Application to Data
MC ε 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 v2in participant plane
corrected to PP
Data Corrected to <v2>published
Ollitrault, Poskanzer, and Voloshin, PRC 80, 014904 (2009)
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corrected to RP
v2 in the Reaction Plane
in Gaussian fluctuation approximation:
Voloshin, Poskanzer, Tang, and Wang, Phys. Lett. B 659, 537 (2008)
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New Results
● Direct Cumulants● Non-Gaussian behavior
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Participant PlaneGlauber CGC
STAR preliminarySTAR preliminary
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Reaction Plane
Glauber CGC
STAR preliminarySTAR preliminary
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Can 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 εpart to εstd
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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CGC
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 εpart Distributions
Non-Gaussian for peripheral collisions
Gaussian and Bessel-Gaussian fits to the black calculations
Hiroshi Masui
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εpart < 1
ε can not be greater than 1
Hiroshi Masui
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Status● 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}● 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