Weak LQG metrics and Liouville first passage percolation

Abstract For $$\gamma \in (0,2)$$γ∈(0,2), we define a weak$$\gamma $$γ-Liouville quantum gravity (LQG) metric to be a function $$h\mapsto D_h$$h↦Dh which takes in an instance of the planar Gaussian free field and outputs a metric on the plane satisfying a certain list of natural axioms. We show tha...

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Päätekijät: Dubédat, Julien, Falconet, Hugo, Gwynne, Ewain, Pfeffer, Joshua, Sun, Xin
Muut tekijät: Massachusetts Institute of Technology. Department of Mathematics
Aineistotyyppi: Artikkeli
Kieli:English
Julkaistu: Springer Berlin Heidelberg 2021
Linkit:https://hdl.handle.net/1721.1/131625
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author Dubédat, Julien
Falconet, Hugo
Gwynne, Ewain
Pfeffer, Joshua
Sun, Xin
author2 Massachusetts Institute of Technology. Department of Mathematics
author_facet Massachusetts Institute of Technology. Department of Mathematics
Dubédat, Julien
Falconet, Hugo
Gwynne, Ewain
Pfeffer, Joshua
Sun, Xin
author_sort Dubédat, Julien
collection MIT
description Abstract For $$\gamma \in (0,2)$$γ∈(0,2), we define a weak$$\gamma $$γ-Liouville quantum gravity (LQG) metric to be a function $$h\mapsto D_h$$h↦Dh which takes in an instance of the planar Gaussian free field 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 et al. (Tightness of Liouville first passage percolation for $$\gamma \in (0,2)$$γ∈(0,2), 2019. ArXiv e-prints, arXiv:1904.08021). It is also known that these axioms are satisfied for the $$\sqrt{8/3}$$8/3-LQG metric constructed by Miller and Sheffield (2013–2016). For any weak $$\gamma $$γ-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-Hölder continuous with respect to the Euclidean metric and compute the optimal Hölder 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 $$\gamma $$γ-LQG metric is unique for each $$\gamma \in (0,2)$$γ∈(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 $$\gamma =\sqrt{8/3}$$γ=8/3.
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spelling mit-1721.1/1316252023-01-20T21:33:32Z Weak LQG metrics and Liouville first passage percolation Dubédat, Julien Falconet, Hugo Gwynne, Ewain Pfeffer, Joshua Sun, Xin Massachusetts Institute of Technology. Department of Mathematics Abstract For $$\gamma \in (0,2)$$γ∈(0,2), we define a weak$$\gamma $$γ-Liouville quantum gravity (LQG) metric to be a function $$h\mapsto D_h$$h↦Dh which takes in an instance of the planar Gaussian free field 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 et al. (Tightness of Liouville first passage percolation for $$\gamma \in (0,2)$$γ∈(0,2), 2019. ArXiv e-prints, arXiv:1904.08021). It is also known that these axioms are satisfied for the $$\sqrt{8/3}$$8/3-LQG metric constructed by Miller and Sheffield (2013–2016). For any weak $$\gamma $$γ-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-Hölder continuous with respect to the Euclidean metric and compute the optimal Hölder 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 $$\gamma $$γ-LQG metric is unique for each $$\gamma \in (0,2)$$γ∈(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 $$\gamma =\sqrt{8/3}$$γ=8/3. 2021-09-20T17:29:06Z 2021-09-20T17:29:06Z 2020-06-18 2020-06-26T12:35:10Z Article http://purl.org/eprint/type/JournalArticle https://hdl.handle.net/1721.1/131625 PUBLISHER_CC en https://doi.org/10.1007/s00440-020-00979-6 Creative Commons Attribution https://creativecommons.org/licenses/by/4.0/ The Author(s) application/pdf Springer Berlin Heidelberg Springer Berlin Heidelberg
spellingShingle Dubédat, Julien
Falconet, Hugo
Gwynne, Ewain
Pfeffer, Joshua
Sun, Xin
Weak LQG metrics and Liouville first passage percolation
title Weak LQG metrics and Liouville first passage percolation
title_full Weak LQG metrics and Liouville first passage percolation
title_fullStr Weak LQG metrics and Liouville first passage percolation
title_full_unstemmed Weak LQG metrics and Liouville first passage percolation
title_short Weak LQG metrics and Liouville first passage percolation
title_sort weak lqg metrics and liouville first passage percolation
url https://hdl.handle.net/1721.1/131625
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