Weak Liouville quantum gravity metrics with matter central charge $\mathbf{c} \in (-\infty, 25)$

Abstract

Physics considerations suggest that a theory of Liouville quantum gravity (LQG) should exist for all values of matter central charge $\mathbf{c} \in (-\infty,25)$. Probabilists have rigorously defined LQG as a random metric measure space for $\mathbf{c} < 1$; however, they have only very recently begun to explore LQG in the $\mathbf{c} \in (1,25)$ phase. We define a random metric associated to LQG for all $\mathbf{c} < 25$ by a collection of axioms analogous to axioms stated in the $\mathbf{c} < 1$ setting. We show that such a metric exists for each $\mathbf{c}$ by considering an approximating metric known as Liouville first passage percolation. Ding and Gwynne proved that these approximating metrics are tight in a suitably chosen topology; we show that every subsequential limit satisfies our axioms. In particular, our result defines a metric associated to LQG in the critical case $\mathbf{c} =1$. The metrics we define for $\mathbf{c} \in (1,25)$ exhibit geometric behavior that sharply contrasts with the $\mathbf{c} < 1$ regime. We show that, for $\mathbf{c} \in (1,25)$, the metrics do not induce the Euclidean topology since they a.s. have a dense (measure zero) set of singular points, points at infinite distance from all other points. We use this fact to prove that a.s. the metric ball is not compact and its boundary has infinite Hausdorff dimension. Despite these differences, we demonstrate that many properties of LQG metrics for $\mathbf{c} < 1$ extend in some form to the entire range $(-\infty, 25)$. We show that the metrics are a.s. reverse Hölder continuous with respect to the Euclidean metric, are a.s. complete and geodesic away from the set of singular points, and satisfy the bounds for set-to-set distances that hold in the $\mathbf{c} < 1$ phase. Finally, we prove that the metrics satisfy a version of the (geometric) Knizhnik-Polyakov-Zamolodchikov (KPZ) formula.

Figures (1)

• Figure 1: Table of relationships between the values of the matter central charge $\operatorname{\mathbf{c}}$, the background charge $Q$, and the coupling constant $\gamma$. When ${\color{black}{\operatorname{\mathbf{c}} \in (-\infty,1]}}$, all three parameters are real. When $\operatorname{\mathbf{c}} \in (1,25)$, $\gamma$ is complex, but $Q$ is real and nonzero.

Theorems & Definitions (5)

• Definition 1.1: Heuristic formulation of LQG
• Definition 1.2
• Definition 1.3
• Definition 1.4
• Definition 1.5