Resummed lattice QCD equation of state at finite baryon density: Strangeness neutrality and beyond

被引:25
|
作者
Borsanyi, Szabolcs [1 ]
Guenther, Jana N. [1 ]
Kara, Ruben [1 ]
Fodor, Zoltan [1 ,2 ,3 ,4 ,5 ]
Parotto, Paolo [2 ]
Pasztor, Attila [3 ]
Ratti, Claudia [6 ]
Szabo, Kalman [1 ,4 ]
机构
[1] Wuppertal Univ, Dept Phys, Gaussstr 20, D-42119 Wuppertal, Germany
[2] Penn State Univ, Dept Phys, University Pk, PA 16802 USA
[3] Eotvos Lorand Univ, Inst Theoret Phys, Pazmany P Setany 1-A, H-1117 Budapest, Hungary
[4] Forschungszentrum Julich, Julich Supercomp Ctr, D-52425 Julich, Germany
[5] Univ Calif San Diego, Phys Dept, San Diego, CA 92093 USA
[6] Univ Houston, Dept Phys, Houston, TX 77204 USA
基金
美国国家科学基金会;
关键词
PHASE-DIAGRAM; TEMPERATURE;
D O I
10.1103/PhysRevD.105.114504
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We calculate a resummed equation of state with lattice QCD simulations at imaginary chemical potentials. This work presents a generalization of the scheme introduced in [Phys. Rev. Lett. 126, 232001 (2021) to the case of nonzero mu(s), focusing on the line of strangeness neutrality. We present results up to mu(B)/T <= 3.5 on the strangeness neutral line < S > = 0 in the temperature range 130 MeV <= T <= 280 MeV. We also extrapolate the finite baryon density equation of state to small nonzero values of the strangeness-to-baryon ratio R = < S > / < B >. We perform a continuum extrapolation using lattice simulations of the 4stout-improved staggered action with 8, 10, 12 and 16 time slices.
引用
收藏
页数:16
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