event-by-event charge/neutral fluctuation at rhic-phenix

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9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 1 Event-by-event charge/neutral fluctuation at RHIC- PHENIX Tomoaki Nakamura / Kensuke Homma Hiroshima University for the PHENIX collaboration

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Event-by-event charge/neutral fluctuation at RHIC-PHENIX. Tomoaki Nakamura / Kensuke Homma Hiroshima University for the PHENIX collaboration. Why fluctuation ?. Measure maximum deviation size in homogeneous flux in our method. The Microwave Sky image from the WMAP Mission - PowerPoint PPT Presentation

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Page 1: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 1

Event-by-event charge/neutral fluctuation at RHIC-PHENIX

Tomoaki Nakamura / Kensuke Homma

Hiroshima University

for the PHENIX collaboration

Page 2: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 2

Why fluctuation ?• Fluctuations carries

information at early universe in cosmology despite of the only single Big-Bang event.

• Why don’t we use the genuine event-by-event information by getting all phase space information to study evolution of dynamical system in Heavy Ion collisions ?

• We can firmly search for interesting fluctuations with more than million times of mini Big-Bangs.

The Microwave Sky image from the WMAP Mission http://map.gsfc.nasa.gov/m_mm.html

Measure maximum deviation size in homogeneous flux in our method

Page 3: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 3

Physics motivation

WMAP have seen the fluctuation of CMB at the recombination.

Fluctuation of charged and neutralπ as charge/neutral balance is a possible probe to extract information at the chiral phase transition (…DCC scenario).

Hadronization

Page 4: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 4

Au+Au √sNN = 200GeV at PHENIX

• Using magnetic field-off• Charged Track

Drift chamber, Pad chamber1 with BBC vertex

• Photon Cluster Electro-magnetic calorimeter– Cluster shower shape– Time of flight– association cuts by tracks

• Precisely data quality assurance was necessary to reject detector effect!

2/1

35.0||

Page 5: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 5

2.4 standard deviation

Charged track

Photon cluster

Event sample and a normal event

Photon clusters

Charged tracks

~3,000 events accumulated

Page 6: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 6

Observable

)(max

)()()(

)()(

)()()(

)()(

)(2)()(

)2,2(

max

)(

22

)(

0

xBB

xBdxxBxB

xNxN

xNxNxB

xNxN

xNxNxB

x

xB

chxB

ch

ch

jj

Balance

0

0

original signal

differential

η,

maximum differential

Page 7: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 7

How to extract region?

η

extract this region

High resolution

Low resolution

Page 8: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 8

High energy cosmic ray experiment and PHENIX

Charged track

Photon cluster

PHENIX 7.24 standard deviation

J. J. Lord and J. Iwai. Int. Conference on High Energy Physics, TX, 1992

○: Photon

+ : Charged Particle

Can DCC scenario explain these events or something else?

Page 9: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 9

Maximum differential balance distributions

Work in Progress

δBmax [arbitrary unit]

• δBmax distribution (each centrality:10%) with base line fluctuation– black : binomial sample,

100 times larger statistics than real data obtained by hit map

– red : data

Page 10: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 10

Work in Progress

[arb

itra

ry u

nit

]

HIJING 1.35 quench on + full reconstruction (67,373 events)

Data M.B. 92.2% (550,426 events)

N-participant dependence of the event fraction above 5% significance level

Page 11: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 11

Summary and plan• Fraction of events above 5% significance level to

exclude binomial fluctuation with respect to minimum bias events increases as N-participants increases.

• Known fluctuations measured by the other experimental observables in our experiment will be parameterized and tested by our observable separately to investigate the source of fluctuations.– Jets : two particle correlations and mean pT fluctuation– Flow effect (would be negligible): V2 analysis– Bose-Einstein correlation : subdivided multiplicity

distributions with Negative Binomial Distribution

Page 12: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 12

Back up slide

Page 13: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 13

Baseline fluctuation

• Yellow band is one of the systematic error coming from ambiguity of limit value as 95% significance level.

• Baseline fluctuation have also a feature of enhancement of fraction at the low multiplicity events and at small resolution level. This algorism can not select large window at the low multiplicity. This is a feature of nature. So we subtracted the baseline fluctuation made by binomial based on hit map.

DATA

base line by binomial sample

5% S.L

after subtraction

Page 14: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 14

level-by-level

Page 15: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 15

wavelet algorism (2 scale relation)

Scaling function

Wavelet function

Level j-1 : 2j-1 bins Level j : 2j bins

φ(2x) = 1/√2 {φ(x) + ψ(x) }φ(2x-1) = 1/√2 {φ(x) - ψ(x) }

-0.7

+0.7

φ(x)

0.7ψ(x)

x

x

-1

1

1

φ(2x-1)

x

-1

1

1

φ(2x)

x

-0.7

Page 16: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 16

Multi resolution analysis

Signal

φ ψ

c jk

d jk

j=4

j=3

j=2

j=1

j=0

j : resolution level (domain size)

k : k-th bin in rapidity

c jk : coefficients of φ

d jk : coefficients of ψ

d jk corresponds tosubtraction between twoneighboring bins exceptscaling factor

k k+

+

+

+

22 20

Page 17: Event-by-event charge/neutral fluctuation at RHIC-PHENIX

9/11/2003 Tomoaki Nakamura - Hiroshima Univ. 17

Window shift

Shift the start bin at eachresolution level.

Find djk max among all of levels.

This can determine the level(domain size) with the largestdeviation size. should appear here !

A symmetric structureappears in wrong level

djk is lower