A distance exponent for Liouville quantum gravity

Abstract

Let γ ∈ (0,2) and let h be the random distribution on C which describes a γ-Liouville quantum gravity (LQG) cone. Also let = 16/γ2 >4 and let η be a whole-plane space-filling SLE curve sampled independent from h and parametrized by γ-quantum mass with respect to h. We study a family \ Gε\ε>0 of planar maps associated with (h, η) called the LQG structure graphs (a.k.a.\ mated-CRT maps) which we conjecture converge in probability in the scaling limit with respect to the Gromov-Hausdorff topology to a random metric space associated with γ-LQG. In particular, Gε is the graph whose vertex set is ε Z, with two such vertices x1,x2∈ ε Z connected by an edge if and only if the corresponding curve segments η([x1-ε , x1]) and η([x2-ε,x2]) share a non-trivial boundary arc. Due to the peanosphere description of SLE-decorated LQG due to Duplantier, Miller, and Sheffield (2014), the graph Gε can equivalently be expressed as an explicit functional of a correlated two-dimensional Brownian motion, so can be studied without any reference to SLE or LQG. We prove non-trivial upper and lower bounds for the cardinality of a graph-distance ball of radius n in Gε which are consistent with the prediction of Watabiki (1993) for the Hausdorff dimension of LQG. Using subadditivity arguments, we also prove that there is an exponent > 0 for which the expected graph distance between generic points in the subgraph of Gε corresponding to the segment η([0,1]) is of order ε- + oε(1), and this distance is extremely unlikely to be larger than ε- + oε(1).

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