有限体积 $2\to2$ 散射中的离散化效应

Maxwell T. Hansen, Toby Peterken
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引用次数: 0

摘要

我们将非零晶格间距效应纳入了L(uscher)的有限体积散射形式主义。新的量化条件将晶格能量作为输入,并返回离散化散射振幅的一个版本,其定义在西曼齐克有效理论中是透明的。与标准形式主义不同,这种方法使用单散点离散化效应来定义有限体积zet函数的修正版本。新形式主义需要两组角动量指数,除了众所周知的红外混合(由于有限体积)之外,还编码了角动量态的紫外混合(由于晶格间距)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Discretization effects in finite-volume $2\to2$ scattering
We incorporate non-zero lattice-spacing effects into L\"uscher's finite-volume scattering formalism. The new quantization condition takes lattice energies as input and returns a version of the discretized scattering amplitude whose definition is transparent in the context of Symanzik Effective Theory. In contrast to the standard formalism, this approach uses single-hadron discretization effects to define modified versions of the finite-volume zeta functions. The new formalism requires two sets of angular-momentum indices, which encode the ultraviolet mixing of angular momentum states (due to the lattice spacing), in addition to the well-known infrared mixing (due to the finite volume).
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