pion number fluctuations and correlations in the statistical system with fixed isospin

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Pion Number Fluctuations and Correlations in the Statistical System with Fixed Isospin V.B., M.I. Gorenstein, O.A. Mogilevsky, Phys. Rev. C 82 (2010) Viktor Begun Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine Frankfurt Institute for Advanced Studies, Frankfurt, Germany

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Pion Number Fluctuations and Correlations in the Statistical System with Fixed Isospin. Viktor Begun Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine Frankfurt Institute for Advanced Studies, Frankfurt, Germany. V.B., M.I. Gorenstein, O.A. Mogilevsky, - PowerPoint PPT Presentation

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Page 1: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Pion Number Fluctuations and Correlations in the

Statistical System with Fixed Isospin

V.B., M.I. Gorenstein, O.A. Mogilevsky,

Phys. Rev. C 82 (2010)

Viktor BegunBogolyubov Institute for Theoretical Physics, Kiev, Ukraine

Frankfurt Institute for Advanced Studies, Frankfurt, Germany

Page 2: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 2/15

Motivation

It was found in 2004 (V.B., Gazdzicki, Gorenstein, Becattini, Ferroni…) that exact conservation of Abelian (additive) charges suppress multiplicity fluctuations even in thermodynamic limit

The aim is to study some aspects of non-Abelian symmetries in the statistical models

Bose – Einstein condensation of pions (V.B., Gorenstein) Phys. Lett. B 2007

Page 3: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 3/15

Partition functions for gas in GCE and CE with Q=0

where z is the

one-particle

partition function

Page 4: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 4/15

CE & GCE

V.B., Gaździcki, Gorenstein, Zozulya, PRC 2004

Mean values, fluctuations and correlations are obta-ined as the derivatives of the corresponding partition function

Page 5: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 5/15

The prediction of hadron gas

V.B., Gazdzicki,Gorenstein, Hauer,

Konchakovski, LungwitzPRC 2006

Small acceptance

< 1 ?!

Page 6: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 6/15

Comparison with the NA49 data

+-

V.B., Gazdzicki, Gorenstein, Hauer, Konchakovski, Lungwitz, PRC 2006

Page 7: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 7/15

The partition function of pion gas with total isospin I=0

Pions are transformed under vector

(adjoint) representation of the SU(2)

group. This group has three para-

meters which can be chosen as

Euler angles. In this case the dia-

gonal matrix elements and the partition function have the following form

Turko and Rafelski, Eur. Phys. J. 2001; Turko, Acta Phys. Polon. 2002

Page 8: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 8/15

The ratio RN and the scaled

variance for total pion number

Page 9: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 9/15

The ratios and Fluctuations of mesons

Isospin conservation generates correlations between the number of neutral and charged pions.

Page 10: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 10/15

Correlation coefficient:

has the value

In the GCE all correlation coefficients

are equal to zero

In the CE

Correlations of mesons

Page 11: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 11/15

Bose Statistics

In the thermodynamic

limitfor Boltzmann statistics:

and for Bose statistics:

Page 12: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 12/15

Bose-Einstein Condensation of pions

We propose to search for the BEC in high multiplicity events of high-energy particle and/or nuclei collisions

Anomalous fluctuation of neutral and charged pions will indicate BEC

Page 13: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 13/15

One way or another, an increase of leads to a strong increase of the fluctuationsof and numbers due to the BEC effects

Fluctuation of 0 – mesons for Q=0, Nπ= const, E=const

Nikitin, Kokoulina,

IHEP, Protvino (Russia)

V.B., Gorenstein, PLB 2007, PRC 2008

Page 14: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 14/15

Summary:

1. For neutral pions there is the enhancement of the fluctuations. For charged pions the isospin conservation suppresses fluctuations similar to that in the CE with Q=0.

2. The positive correlations between the numbers of neutral and positive (negative) pions are observed for I=0.

3. The colorless system of SU(2)-color gluons corresponds to the I=0 pion gas. We thus conclude that fluctuations of the number of gluons with different colors are different. This difference survives in the thermodynamic limit.

Page 15: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

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Bose-Einstein Corelation

Condensation ?

arXiv:1007.0516v1

Page 16: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 16/15

Phase diagram

V.B., M.I. Gorenstein, Phys. Lett. B (2007), Phys. Rev C (2008)

Project THERMALIZATION

Page 17: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 17/15

Pais, Annals Phys. 1960

The degeneracy factors

Page 18: Pion Number  Fluctuations  and  Correlations  in the Statistical System with Fixed  Isospin

Viktor Begun 18/15

The partition function of pion gas with total isospin I=0

The change of variables and integration gives:

The final expressions for the partition

functions correspond to .

Taking the derivatives of Z over T

and V one obtains the thermody-

namical functions of the system.