# Weak LQG metrics and Liouville first passage percolation

## TL;DR

This paper defines and analyzes weak Liouville quantum gravity (LQG) metrics, establishing their properties, bounds, and regularity, and demonstrating their relation to Liouville first passage percolation limits, with implications for metric uniqueness.

## Contribution

It introduces a framework for weak LQG metrics satisfying natural axioms, proves their properties, and connects them to Liouville first passage percolation subsequential limits, advancing understanding of LQG geometry.

## Key findings

- Weak $eta$-LQG metrics satisfy natural axioms.
- Derived moment bounds for diameters and distances.
- Established local bi-Hölder continuity and optimal exponents.

## Abstract

For $\gamma \in (0,2)$, we define a weak $\gamma$-Liouville quantum gravity (LQG) metric to be a function $h\mapsto D_h$ which takes in an instance of the planar Gaussian free field (GFF) and outputs a metric on the plane satisfying a certain list of natural axioms. We show that these axioms are satisfied for any subsequential limits of Liouville first passage percolation. Such subsequential limits were proven to exist by Ding-Dub\'edat-Dunlap-Falconet (2019). It is also known that these axioms are satisfied for the $\sqrt{8/3}$-LQG metric constructed by Miller and Sheffield (2013-2016). For any weak $\gamma$-LQG metric, we obtain moment bounds for diameters of sets as well as point-to-point, set-to-set, and point-to-set distances. We also show that any such metric is locally bi-H\"older continuous with respect to the Euclidean metric and compute the optimal H\"older exponents in both directions. Finally, we show that LQG geodesics cannot spend a long time near a straight line or the boundary of a metric ball. These results are used in subsequent work by Gwynne and Miller which proves that the weak $\gamma$-LQG metric is unique for each $\gamma \in (0,2)$, which in turn gives the uniqueness of the subsequential limit of Liouville first passage percolation. However, most of our results are new even in the special case when $\gamma=\sqrt{8/3}$.