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dc.contributor.authorGwynne, Ewain
dc.contributor.authorHolden, Nina
dc.contributor.authorSun, Xin
dc.date.accessioned2021-09-20T17:17:05Z
dc.date.available2021-09-20T17:17:05Z
dc.date.issued2018-04-26
dc.identifier.urihttps://hdl.handle.net/1721.1/131438
dc.description.abstractAbstract Let $$\gamma \in (0,2)$$ γ ∈ ( 0 , 2 ) and let h be the random distribution on $$\mathbb C$$ C which describes a $$\gamma $$ γ -Liouville quantum gravity (LQG) cone. Also let $$\kappa = 16/\gamma ^2 >4$$ κ = 16 / γ 2 > 4 and let $$\eta $$ η be a whole-plane space-filling SLE $$_\kappa $$ κ curve sampled independent from h and parametrized by $$\gamma $$ γ -quantum mass with respect to h. We study a family $$\{\mathcal G^\epsilon \}_{\epsilon >0}$$ { G ϵ } ϵ > 0 of planar maps associated with $$(h, \eta )$$ ( 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 $$\gamma $$ γ -LQG. In particular, $$\mathcal G^\epsilon $$ G ϵ is the graph whose vertex set is $$\epsilon \mathbb Z$$ ϵ Z , with two such vertices $$x_1,x_2\in \epsilon \mathbb Z$$ x 1 , x 2 ∈ ϵ Z connected by an edge if and only if the corresponding curve segments $$\eta ([x_1-\epsilon , x_1])$$ η ( [ x 1 - ϵ , x 1 ] ) and $$\eta ([x_2-\epsilon ,x_2])$$ η ( [ x 2 - ϵ , x 2 ] ) share a non-trivial boundary arc. Due to the peanosphere description of SLE-decorated LQG due to Duplantier et al. (Liouville quantum gravity as a mating of trees, 2014), the graph $$\mathcal G^\epsilon $$ G ϵ 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 $$\mathcal G^\epsilon $$ G ϵ which are consistent with the prediction of Watabiki (Prog Theor Phys Suppl 114:1–17, 1993) for the Hausdorff dimension of LQG. Using subadditivity arguments, we also prove that there is an exponent $$\chi > 0$$ χ > 0 for which the expected graph distance between generic points in the subgraph of $$\mathcal G^\epsilon $$ G ϵ corresponding to the segment $$\eta ([0,1])$$ η ( [ 0 , 1 ] ) is of order $$\epsilon ^{-\chi + o_\epsilon (1)}$$ ϵ - χ + o ϵ ( 1 ) , and this distance is extremely unlikely to be larger than $$\epsilon ^{-\chi + o_\epsilon (1)}$$ ϵ - χ + o ϵ ( 1 ) .en_US
dc.publisherSpringer Berlin Heidelbergen_US
dc.relation.isversionofhttps://doi.org/10.1007/s00440-018-0846-9en_US
dc.rightsArticle is made available in accordance with the publisher's policy and may be subject to US copyright law. Please refer to the publisher's site for terms of use.en_US
dc.sourceSpringer Berlin Heidelbergen_US
dc.titleA distance exponent for Liouville quantum gravityen_US
dc.typeArticleen_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Mathematics
dc.eprint.versionAuthor's final manuscripten_US
dc.type.urihttp://purl.org/eprint/type/JournalArticleen_US
eprint.statushttp://purl.org/eprint/status/PeerRevieweden_US
dc.date.updated2020-09-24T20:57:54Z
dc.language.rfc3066en
dc.rights.holderSpringer-Verlag GmbH Germany, part of Springer Nature
dspace.embargo.termsY
dspace.date.submission2020-09-24T20:57:53Z
mit.licensePUBLISHER_POLICY
mit.metadata.statusAuthority Work and Publication Information Needed


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