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Path Integral Quantization of Volume
Annales Henri Poincaré ( IF 1.5 ) Pub Date : 2020-01-10 , DOI: 10.1007/s00023-019-00882-4
Adrian P. C. Lim

A hyperlink is a finite set of non-intersecting simple closed curves in \(\mathbb {R} \times \mathbb {R}^3\). Let R be a compact set inside \(\mathbb {R}^3\). The dynamical variables in General Relativity are the vierbein e and a \(\mathfrak {su}(2)\times \mathfrak {su}(2)\)-valued connection \(\omega \). Together with Minkowski metric, e will define a metric g on the manifold. Denote \(V_R(e)\) as the volume of R, for a given choice of e. The Einstein–Hilbert action \(S(e,\omega )\) is defined on e and \(\omega \). We will quantize the volume of R by integrating \(V_R(e)\) against a holonomy operator of a hyperlink L, disjoint from R, and the exponential of the Einstein–Hilbert action, over the space of vierbein e and \(\mathfrak {su}(2)\times \mathfrak {su}(2)\)-valued connection \(\omega \). Using our earlier work done on Chern–Simons path integrals in \(\mathbb {R}^3\), we will write this infinite-dimensional path integral as the limit of a sequence of Chern–Simons integrals. Our main result shows that the volume operator can be computed by counting the number of nodes on the projected hyperlink in \(\mathbb {R}^3\), which lie inside the interior of R. By assigning an irreducible representation of \(\mathfrak {su}(2)\times \mathfrak {su}(2)\) to each component of L, the volume operator gives the total kinetic energy, which comes from translational and angular momentum.

中文翻译:

体积的路径积分量化

超链接是\(\ mathbb {R} \ times \ mathbb {R} ^ 3 \)中有限的一组非相交的简单闭合曲线。令R\(\ mathbb {R} ^ 3 \)内部的紧集。广义相对论中的动力学变量是vierbein e\(\ mathfrak {su}(2)\ times \ mathfrak {su}(2)\)值连接\(\ omega \)e与Minkowski度量一起在流形上定义度量g。表示\(V_R(E)\)作为的体积- [R ,对于一个给定的选择ë。爱因斯坦–希尔伯特动作\(S(e,\ omega)\)e\(\ omega \)。我们将通过对超级链接L的完整算术运算符\(V_R(e)\)积分R R不相交)以及Einstein–Hilbert作用的指数,在verbein e\(\ mathfrak {su}(2)\ times \ mathfrak {su}(2)\)值连接\(\ omega \)。使用我们先前在\(\ mathbb {R} ^ 3 \)中对Chern–Simons路径积分所做的工作,我们将把这个无限维路径积分写为Chern–Simons积分序列的极限。我们的主要结果表明,可以通过计算投影超链接中的节点数来计算体积算符\(\ mathbb {R} ^ 3 \),它位于R的内部。通过为L的每个分量分配\(\ mathfrak {su}(2)\ times \ mathfrak {su}(2)\)的不可约表示,体积算子给出了总动能,该动能来自平动和角动量。
更新日期:2020-01-10
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