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首页> 外文期刊>Physical review, D >Self-consistency and covariance of light-front quark models: Testing via P, V, and A meson decay constants, and P→P weak transition form factors
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Self-consistency and covariance of light-front quark models: Testing via P, V, and A meson decay constants, and P→P weak transition form factors

机译:光前夸克模型的自洽和协方差:通过P,V和A介子衰变常数以及P→P弱跃迁形状因子进行测试

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In this paper, we test the self-consistencies of the standard and the covariant light-front quark model and study the zero-mode issue via the decay constants of pseudoscalar ( P ), vector ( V ) and axial-vector ( A ) mesons, as well as the P → P weak transition form factors. With the traditional type-I correspondence between the manifestly covariant and the light-front approach, the resulting f V as well as f A 1 and f A 3 obtained with the λ = 0 and λ = ± polarization states are different from each other, which presents a challenge to the self-consistency of the covariant light-front quark model. However, such a self-consistency problem can be “resolved” within the type-II scheme, which requires an additional replacement M → M 0 relative to the type-I case. Moreover, the replacement M → M 0 is also essential for the self-consistency of the standard light-front quark model. In the type-II scheme, the valence contributions to the physical quantities ( Q ) considered in this paper are always the same as that obtained in the standard light-front quark model, [ Q ] val = [ Q ] SLF , and the zero-mode contributions to f V , 1 A , 3 A and f ? ( q 2 ) exist only formally but vanish numerically, which further implies that [ Q ] val = ˙ [ Q ] full . In addition, the manifest covariance of the covariant light-front quark model is violated in the traditional type-I scheme, but can be recovered by taking the type-II correspondence.
机译:在本文中,我们测试了标准和协变光前夸克模型的自洽性,并通过伪标量(P),矢量(V)和轴向矢量(A)介子的衰减常数研究零模问题。 ,以及P→P的弱过渡形状因子。利用明显的协变和光前方法之间的传统I型对应关系,得到的f V以及在λ= 0和λ=±偏振态下获得的f A 1和f A 3互不相同,这对协变光前夸克模型的自洽性提出了挑战。但是,这样的自洽问题可以在II型方案中“解决”,相对于I型方案,这需要额外的替换M→M 0。此外,替换M→M 0对于标准光前夸克模型的自洽性也是必不可少的。在II型方案中,本文考虑的化合价对物理量(Q)的贡献始终与在标准光前夸克模型中获得的化合价[Q] val = [Q] SLF相同,零模式对f V,1 A,3 A和f的贡献? (q 2)仅形式上存在,但数值上消失,这进一步意味着[Q] val =˙[Q] full。另外,在传统的I型方案中违反了协变光前夸克模型的明显协方差,但是可以通过采用II型对应关系来恢复。

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