Fluctuations and correlations of net baryon number, electric charge, and strangeness: A comparison of lattice QCD results with the hadron resonance gas model

A. Bazavov, Tanmoy Bhattacharya, C. E. DeTar, H.-T. Ding, Steven Gottlieb, Rajan Gupta, P. Hegde, Urs M. Heller, F. Karsch, E. Laermann, L. Levkova, Swagato Mukherjee, P. Petreczky, Christian Schmidt, R. A. Soltz, W. Soeldner, R. Sugar, and Pavlos M. Vranas (HotQCD Collaboration)
Phys. Rev. D 86, 034509 – Published 31 August 2012

Abstract

We calculate the quadratic fluctuations of net baryon number, electric charge and strangeness as well as correlations among these conserved charges in (2+1)-flavor lattice QCD at zero chemical potential. Results are obtained using calculations with tree-level improved gauge and the highly improved staggered quark actions with almost physical light and strange quark masses at three different values of the lattice cutoff. Our choice of parameters corresponds to a value of 160 MeV for the lightest pseudoscalar Goldstone mass and a physical value of the kaon mass. The three diagonal charge susceptibilities and the correlations among conserved charges have been extrapolated to the continuum limit in the temperature interval 150MeVT250MeV. We compare our results with the hadron resonance gas (HRG) model calculations and find agreement with HRG model results only for temperatures T150MeV. We observe significant deviations in the temperature range 160MeVT170MeV and qualitative differences in the behavior of the three conserved charge sectors. At T160MeV quadratic net baryon number fluctuations in QCD agree with HRG model calculations, while the net electric charge fluctuations in QCD are about 10% smaller and net strangeness fluctuations are about 20% larger. These findings are relevant to the discussion of freeze-out conditions in relativistic heavy ion collisions.

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  • Received 7 March 2012

DOI:https://doi.org/10.1103/PhysRevD.86.034509

© 2012 American Physical Society

Authors & Affiliations

A. Bazavov1, Tanmoy Bhattacharya2, C. E. DeTar3, H.-T. Ding1, Steven Gottlieb4, Rajan Gupta2, P. Hegde1, Urs M. Heller5, F. Karsch1,6, E. Laermann6, L. Levkova3, Swagato Mukherjee1, P. Petreczky1, Christian Schmidt6, R. A. Soltz7, W. Soeldner8, R. Sugar9, and Pavlos M. Vranas7 (HotQCD Collaboration)

  • 1Physics Department, Brookhaven National Laboratory, Upton, New York 11973, USA
  • 2Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
  • 3Department of Physics and Astronomy, University of Utah, Salt Lake City, Utah 84112, USA
  • 4Physics Department, Indiana University, Bloomington, Indiana 47405, USA
  • 5American Physical Society, One Research Road, Ridge, New York 11961, USA
  • 6Fakultät für Physik, Universität Bielefeld, D-33615 Bielefeld, Germany
  • 7Physics Division, Lawrence Livermore National Laboratory, Livermore California 94550, USA
  • 8Institut für Theoretische Physik, Universität Regensburg, D-93040 Regensburg, Germany
  • 9Physics Department, University of California, Santa Barbara, California 93106, USA

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Issue

Vol. 86, Iss. 3 — 1 August 2012

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