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Spontaneous chiral-symmetry breaking of lattice QCD with massless dynamical quarks

机译:无质量动力学夸克的晶格QCD自发对称分裂

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摘要

One of the most challenging issues in QCD is the investigation of spontaneous chiral-symmetry breaking, which is characterized by the non-vanishing chiral condensate when the bare fermion mass is zero. In standard methods of the lattice gauge theory, one has to perform expensive simulations at multiple bare quark masses, and employ some modeled functions to extrapolate the data to the chiral limit. This paper applies the probability distribution function method to computing the chiral condensate in lattice QCD with massless dynamical quarks, without any ambiguous mass extrapolation. The results for staggered quarks indicate that this might be a promising and efficient method for investigating the spontaneous chiral-symmetry breaking in lattice QCD, which deserves further investigation.
机译:QCD中最具挑战性的问题之一是自发手性对称性断裂的研究,其特征是当裸费米子质量为零时手性缩合物不消失。在晶格规理论的标准方法中,必须在多个裸夸克质量上执行昂贵的模拟,并采用一些建模函数将数据外推至手性极限。本文采用概率分布函数法在无质量动力学夸克的情况下,在无任何质量外推的情况下,计算出了具有无质量动力学夸克的晶格QCD中的手性缩合物。交错夸克的结果表明,这可能是研究晶格QCD中自发手性对称性断裂的有前途和有效的方法,值得进一步研究。

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