EPJ Web Conf.
Volume 137, 2017XIIth Quark Confinement and the Hadron Spectrum
|Number of page(s)||8|
|Section||Section D: Deconfinement|
|Published online||22 March 2017|
Study of lattice QCD at finite baryon density using the canonical approach
1 Institute for High Energy Physics NRC “Kurchatov Institute”, 142281 Protvino, Russia
2 Institute for Theoretical and Experimental Physics NRC “Kurchatov Institute”, 117218 Moscow, Russia
3 School of Biomedicine, Far Eastern Federal University, 690950 Vladivostok, Russia
4 School of Natural Sciences, Far Eastern Federal University, 690950 Vladivostok, Russia
5 Research Center for Nuclear Physics (RCNP), Osaka University, Ibaraki, Osaka, 567-0047, Japan
6 Theoretical Research Division, Nishina Center, RIKEN, Wako 351-0198, Japan
7 Moscow Institute of Physics and Technology, 141700 Dolgoprudny, Moscow Region, Russia
a e-mail: firstname.lastname@example.org
Published online: 22 March 2017
At finite baryon density lattice QCD first-principle calculations can not be performed due to the sign problem. In order to circumvent this problem, we use the canonical approach, which provides reliable analytical continuation from the imaginary chemical potential region to the real chemical potential region. We briefly present the canonical partition function method, describe our formulation, and show the results, obtained for two temperatures: T/Tc = 0:93 and T/Tc = 0:99 in lattice QCD with two flavors of improved Wilson fermions.
© The Authors, published by EDP Sciences, 2017
This is an Open Access article distributed under the terms of the Creative Commons Attribution License 4.0, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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