带边界的杨-米尔斯理论的辛约简:从超选择扇区到边缘模式,再返回

A. Riello
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引用次数: 7

摘要

我发展了一种适用于杨密理论和电磁学中有界区域的辛约化理论。在这个理论中,电通量的超选择扇区起着中心作用。在给定的超选择扇区内,简化Yang-Mills理论的辛结构总是可以在不包含新自由度的情况下定义,但它是先验的,不是唯一的。然后考虑在所有超选择扇区的并集上定义一个辛结构的可能性。这反过来又需要包括额外的边界自由度,即“边缘模式”。然而,除非新的边缘模式模拟了位于区域边界的材料物理系统,否则我认为边缘模式的相空间扩展也具有固有的模糊性。在超选择和边缘模式框架中,模糊性都可以理解为由于边界的存在而产生的残余量规固定依赖——这一结果与具有渐近边界的QED中的发现相一致。最后,我将比较和对比超选择和边缘模式框架。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Symplectic reduction of Yang-Mills theory with boundaries: from superselection sectors to edge modes, and back
I develop a theory of symplectic reduction that applies to bounded regions in Yang-Mills theory and electromagnetism. In this theory superselection sectors for the electric-flux play a central role. Within a given superselection sector, the symplectic structure of the reduced Yang-Mills theory can always be defined without inclusion of new degrees of freedom, but is a priori not unique. I then consider the possibility of defining a symplectic structure on the union of all superselection sectors. This in turn requires including additional boundary degrees of freedom aka "edge modes." However, unless the new edge modes model a material physical system located at the boundary of the region, I argue that the the phase space extension by edge modes is also inherently ambiguous. In both the superselection and edge mode frameworks, the ambiguity can be understood as a residual gauge-fixing dependence due to the presence of boundaries -- a result that resonates with findings in QED with asymptotic boundaries. To conclude, I will compare and contrast the superselection and edge mode frameworks.
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