Differential Geometry on the Space of Connections via Graphs and Projective Limits
Abhay Ashtekar, Jerzy Lewandowski
TL;DR
The paper develops a metric-free differential geometry on the quantum configuration space $\overline{{\cal A}/{\cal G}}$, obtained as a projective limit of graphs labeling compact manifolds. It constructs differential forms, vector fields, volume forms, and momentum operators on the upstairs space $\overline{\cal A}$ and descends invariantly to the quotient $\overline{{\cal A}/{\cal G}}$, all without a background metric. By introducing edge-metrics $l$ and natural co-metrics $k_{o}$, it defines Laplacians $\Delta_{(l)}$ and $\Delta^{o}$ and associated heat-kernel measures that respect diffeomorphism invariance. The framework also handles non-compact structure groups and discusses extensions to quantum gravity via diffeomorphism-invariant measures and connections to non-perturbative loop-quantum gravity concepts. Overall, the work provides a robust algebraic-geometric toolkit for analyzing gauge theories in a background-independent setting, with concrete operators and measures that can underpin rigorous treatments of quantum gravity.
Abstract
In a quantum mechanical treatment of gauge theories (including general relativity), one is led to consider a certain completion, $\agb$, of the space $\ag$ of gauge equivalent connections. This space serves as the quantum configuration space, or, as the space of all Euclidean histories over which one must integrate in the quantum theory. $\agb$ is a very large space and serves as a ``universal home'' for measures in theories in which the Wilson loop observables are well-defined. In this paper, $\agb$ is considered as the projective limit of a projective family of compact Hausdorff manifolds, labelled by graphs (which can be regarded as ``floating lattices'' in the physics terminology). Using this characterization, differential geometry is developed through algebraic methods. In particular, we are able to introduce the following notions on $\agb$: differential forms, exterior derivatives, volume forms, vector fields and Lie brackets between them, divergence of a vector field with respect to a volume form, Laplacians and associated heat kernels and heat kernel measures. Thus, although $\agb$ is very large, it is small enough to be mathematically interesting and physically useful. A key feature of this approach is that it does not require a background metric. The geometrical framework is therefore well-suited for diffeomorphism invariant theories such as quantum general relativity.
