Discrete quantum geometries and their effective dimension

TL;DR

This thesis investigates how discrete quantum geometries in quantum gravity approaches can give rise to smooth classical spacetimes, focusing on effective dimension measures like spectral dimension and their dependence on combinatorial structure.

Contribution

It provides a combinatorial framework for discrete quantum geometries, extends group field theory, and introduces a discrete calculus to analyze effective dimensions in quantum gravity models.

Findings

Spectral dimension is more sensitive to combinatorial structure than geometric data.

Semiclassical states approximate classical geometries well with no strong quantum effects.

Spectral dimension flows from topological dimension to a lower value at high energies, indicating fractal-like quantum geometries.

Abstract

In several approaches towards a quantum theory of gravity, such as group field theory and loop quantum gravity, quantum states and histories of the geometric degrees of freedom turn out to be based on discrete spacetime. The most pressing issue is then how the smooth geometries of general relativity, expressed in terms of suitable geometric observables, arise from such discrete quantum geometries in some semiclassical and continuum limit. In this thesis I tackle the question of suitable observables focusing on the effective dimension of discrete quantum geometries. For this purpose I give a purely combinatorial description of the discrete structures which these geometries have support on. As a side topic, this allows to present an extension of group field theory to cover the combinatorially larger kinematical state space of loop quantum gravity. Moreover, I introduce a discrete calculus for fields on such fundamentally discrete geometries with a particular focus on the Laplacian. This permits to define the effective-dimension observables for quantum geometries. Analysing various classes of quantum geometries, I find as a general result that the spectral dimension is more sensitive to the underlying combinatorial structure than to the details of the additional geometric data thereon. Semiclassical states in loop quantum gravity approximate the classical geometries they are peaking on rather well and there are no indications for stronger quantum effects. On the other hand, in the context of a more general model of states which are superposition over a large number of complexes, based on analytic solutions, there is a flow of the spectral dimension from the topological dimension $d$ on low energy scales to a real number $0<\alpha<d$ on high energy scales. In the particular case of $\alpha=1$ these results allow to understand the quantum geometry as effectively fractal.