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arXiv 1504.02170math-phgr-qchep-thmath.MP
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相干态,量子引力和玻恩-奥本海默近似,II:紧致李群

Coherent states, quantum gravity and the Born-Oppenheimer approximation, II: Compact Lie Groups

Alexander Stottmeister, Thomas Thiemann

摘要:

在这篇文章中,第二个三,我们讨论和发展的基础外尔量子化的紧李群,旨在圈量子引力型模型。这种外尔量子化可以作为在这种模型中实现空间绝热微扰理论程序的主要数学工具。正如我们在第一篇文章中已经讨论过的,空间绝热微扰理论提供了一个理想的框架,可以克服在圈量子引力的正则形式中直接实现传统的玻恩-奥本海默方法的障碍。此外,我们猜想存在一种新形式的Segal-Bargmann-Hall“相干态”变换的紧凑李群$G$,我们证明了$G=U(1)^{n}$和支持的数值证据$G=SU(2)$。将这一猜想与本文的主要主题结合起来的原因源于观察,即相干态变换可以用作紧致李群$G$的相干态量子化(Berezin量子化)的基本构建块。但是,由于$\mathbb{R}^{2d}$的Weyl和Berezin量子化与热核演化密切相关,很自然地会问,紧李群是否也存在类似的联系。此外,由于制定的空间绝热微扰理论需要(变形)量子化作为最小的输入,我们分析的问题在何种程度上的相干态量子化,定义的Segal-Bargmann-Hall变换,可以作为前者的基础。

英文摘要:

In this article, the second of three, we discuss and develop the basis of a Weyl quantisation for compact Lie groups aiming at loop quantum gravity-type models. This Weyl quantisation may serve as the main mathematical tool to implement the program of space adiabatic perturbation theory in such models. As we already argued in our first article, space adiabatic perturbation theory offers an ideal framework to overcome the obstacles that hinder the direct implementation of the conventional Born-Oppenheimer approach in the canonical formulation of loop quantum gravity. Additionally, we conjecture the existence of a new form of the Segal-Bargmann-Hall "coherent state" transform for compact Lie groups $G$, which we prove for $G=U(1)^{n}$ and support by numerical evidence for $G=SU(2)$. The reason for conjoining this conjecture with the main topic of this article originates in the observation, that the coherent state transform can be used as a basic building block of a coherent state quantisation (Berezin quantisation) for compact Lie groups $G$. But, as Weyl and Berezin quantisation for $\mathbb{R}^{2d}$ are intimately related by heat kernel evolution, it is natural to ask, whether a similar connection exists for compact Lie groups, as well. Moreover, since the formulation of space adiabatic perturbation theory requires a (deformation) quantisation as minimal input, we analyse the question to what extent the coherent state quantisation, defined by the Segal-Bargmann-Hall transform, can serve as basis of the former.

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