The QCD phase diagram for external magnetic fields

被引:572
作者
Bali, G. S. [1 ]
Bruckmann, F. [1 ]
Endrodi, G. [1 ]
Fodor, Z. [2 ,3 ,4 ]
Katz, S. D. [3 ]
Krieg, S. [2 ,4 ]
Schaefer, A. [1 ]
Szabo, K. K. [2 ]
机构
[1] Univ Regensburg, Inst Theoret Phys, D-93040 Regensburg, Germany
[2] Berg Univ Wuppertal, Dept Phys, D-42119 Wuppertal, Germany
[3] Eotvos Lorand Univ, Inst Theoret Phys, H-1117 Budapest, Hungary
[4] Forschungszentrum Julich, Julich Supercomp Ctr, D-52425 Julich, Germany
来源
JOURNAL OF HIGH ENERGY PHYSICS | 2012年 / 02期
关键词
Lattice QCD; Lattice Quantum Field Theory; SYMMETRY-BREAKING; PARITY VIOLATION; NEVEU MODEL; TRANSITION; PARTICLE; TEMPERATURE; CATALYSIS; DEPENDENCE; OPERATOR; MASSES;
D O I
10.1007/JHEP02(2012)044
中图分类号
O412 [相对论、场论]; O572.2 [粒子物理学];
学科分类号
摘要
The effect of an external (electro) magnetic field on the finite temperature transition of QCD is studied. We generate configurations at various values of the quantized magnetic flux with N-f = 2 + 1 flavors of stout smeared staggered quarks, with physical masses. Thermodynamic observables including the chiral condensate and susceptibility, and the strange quark number susceptibility are measured as functions of the field strength. We perform the renormalization of the studied observables and extrapolate the results to the continuum limit using N-t = 6, 8 and 10 lattices. We also check for finite volume effects using various lattice volumes. We find from all of our observables that the transition temperature T c significantly decreases with increasing magnetic field. This is in conflict with various model calculations that predict an increasing T-c(B). From a finite volume scaling analysis we find that the analytic crossover that is present at B = 0 persists up to our largest magnetic fields e B approximate to 1 GeV2, and that the transition strength increases mildly up to this e B approximate to 1 GeV2.
引用
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页数:25
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