Journal
Article title
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Abstracts
We employ the lattice QCD data on Taylor expansion coefficients to extend our previous parametrization of the equation of state to finite baryon density. When we take into account lattice spacing and quark mass dependence of the hadron masses, the Taylor coefficients at low temperature are equal to those of hadron resonance gas. Parametrized lattice equation of state can thus be smoothly connected to the hadron resonance gas equation of state at low temperatures.
Journal
Year
Volume
Issue
Pages
1385-1387
Physical description
Dates
published
1 - 12 - 2012
online
4 - 12 - 2012
Contributors
author
- Institut für Theoretische Physik, Johann Wolfgang Goethe-Universität, 60438, Frankfurt am Main, Germany, huovinen@th.physik.uni-frankfurt.de
author
- Physics Department, Brookhaven National Laboratory, Upton, NY, 11973, USA
author
- Fakultät für Physik, Universität Bielefeld, 33615, Bielefeld, Germany
References
- [1] C. Miao et al. [RBC-Bielefeld Collaboration], PoS LATTICE2008, 172 (2008)
- [2] M. Cheng et al., Phys. Rev. D 79, 074505 (2009) http://dx.doi.org/10.1103/PhysRevD.79.074505[Crossref]
- [3] P. Huovinen, P. Petreczky, Nucl. Phys. A 837, 26 (2010) http://dx.doi.org/10.1016/j.nuclphysa.2010.02.015[Crossref]
- [4] P. Huovinen, P. Petreczky, J. Phys. G 38, 124103 (2011) http://dx.doi.org/10.1088/0954-3899/38/12/124103[Crossref]
- [5] P. Huovinen, P. Petreczky, J. Phys. Conf. Ser. 230, 012012 (2010) http://dx.doi.org/10.1088/1742-6596/230/1/012012[Crossref]
- [6] A. Bazavov et al. [HotQCD Collaboration], J. Phys. Conf. Ser. 230, 012014 (2010) http://dx.doi.org/10.1088/1742-6596/230/1/012014[Crossref]
- [7] D. Teaney, J. Lauret, E. V. Shuryak, arXiv:nuclth/0110037
- [8] C. Schmidt, Eur. Phys. J. C 61, 537 (2009) http://dx.doi.org/10.1140/epjc/s10052-009-0882-9[Crossref]
- [9] P. Huovinen, Nucl. Phys. A 761, 296 (2005) http://dx.doi.org/10.1016/j.nuclphysa.2005.07.016[Crossref]
Document Type
Publication order reference
Identifiers
YADDA identifier
bwmeta1.element.-psjd-doi-10_2478_s11534-012-0110-3