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arXiv 2201.09253hep-phhep-lat
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非零磁场和温度下QCD中的夸克凝聚体

Quark condensate in QCD at nonzero magnetic field and temperature

Yu. A. Simonov

摘要:

本文从考虑禁闭的场方程出发,导出了任意外磁场和温度下夸克凝聚的基本形式。所得到的手性缩合物的表达被示出为在原点处的单线态$q\bar q$基态波函数的平方成比例,$|ϕ_0(0)|^2$。对于没有磁场的轻夸克,凝聚与$σ^{3/2}$成正比($σ$是弦张力)。数值结果在5个表中给出,并且显示出与晶格数据良好的一致性,对于非零磁场$eB$和温度$T$,在$0 <T < 120$ ~MeV,~ $0 <eB <4$ ~GeV $^2$范围内。

英文摘要:

The basic form of the quark condensate for arbitrary values of external magnetic field and temperature, is derived using the field equations with account of confinement. The resulting expression of the chiral condensate is shown to be proportional to square of the singlet $q\bar q$ ground state wave function at origin, $|ϕ_0(0)|^2$. For light quarks without magnetic field the condensates are proportional to $σ^{3/2}$ ($σ$ is the string tension). Numerical results are presented in 5 Tables and shown to be in good agreement with the lattice data, both for nonzero magnetic field $eB$ and temperature $T$ in the range $0 <T < 120$~MeV,~ $0 <eB <4$~GeV$^2$.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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