Abstract
We review and extend the recently proposed model of combinatorial quantum gravity. Contrary to previous discrete approaches, this model is defined on (regular) random graphs and is driven by a purely combinatorial version of Ricci curvature, the Ollivier curvature, defined on generic metric spaces equipped with a Markov chain. It dispenses thus of notions such as simplicial complexes and Regge calculus and is ideally suited to extend quantum gravity to combinatorial structures which have a priori nothing to do with geometry. Indeed, our results show that geometry and general relativity emerge from random structures in a second-order phase transition due to the condensation of cycles on random graphs, a critical point that defines quantum gravity non-perturbatively according to asymptotic safety. In combinatorial quantum gravity the entropy area law emerges naturally as a consequence of infinite-dimensional critical behaviour on networks rather than on lattices. We propose thus that the entropy area law is a signature of the random graph nature of space-(time) on the smallest scales.
Highlights
Ultraviolet (UV) fixed points of statistical mechanics models define renormalizable quantum field theories via the Wilson renormalization group [1]
The asymptotic safety scenario [4] would be realized on networks, rather than traditional statistical mechanics models
In the traditional discrete approach to quantum gravity [5] a smooth background is assumed, which is approximated by piecewise flat geometries on which curvature is computed by Regge calculus [6]
Summary
Ultraviolet (UV) fixed points of statistical mechanics models define renormalizable quantum field theories via the Wilson renormalization group [1]. When equipped with a Markov chain, like a probability measure, a purely combinatorial notion of Ricci curvature, first introduced by Ollivier [7–9], can be defined on such structures. This was used in [2] to define a model of purely combinatorial quantum gravity. This approach was subsequently pursued in [10], where a modified version of the Ollivier curvature was introduced. Gi where the sum runs over all the vertices of the graph and g is a coupling constant with dimension 1/action This expression for the Ollivier curvature still looks forbidding. As we will show in a moment, it will become extremely simple on the physical configuration space
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