{ "id": "0902.3842", "version": "v3", "published": "2009-02-23T03:34:33.000Z", "updated": "2010-10-02T06:40:59.000Z", "title": "Thick points of the Gaussian free field", "authors": [ "Xiaoyu Hu", "Jason Miller", "Yuval Peres" ], "comment": "Published in at http://dx.doi.org/10.1214/09-AOP498 the Annals of Probability (http://www.imstat.org/aop/) by the Institute of Mathematical Statistics (http://www.imstat.org)", "journal": "Annals of Probability 2010, Vol. 38, No. 2, 896-926", "doi": "10.1214/09-AOP498", "categories": [ "math.PR", "math-ph", "math.MP" ], "abstract": "Let $U\\subseteq\\mathbf{C}$ be a bounded domain with smooth boundary and let $F$ be an instance of the continuum Gaussian free field on $U$ with respect to the Dirichlet inner product $\\int_U\\nabla f(x)\\cdot \\nabla g(x)\\,dx$. The set $T(a;U)$ of $a$-thick points of $F$ consists of those $z\\in U$ such that the average of $F$ on a disk of radius $r$ centered at $z$ has growth $\\sqrt{a/\\pi}\\log\\frac{1}{r}$ as $r\\to 0$. We show that for each $0\\leq a\\leq2$ the Hausdorff dimension of $T(a;U)$ is almost surely $2-a$, that $\\nu_{2-a}(T(a;U))=\\infty$ when $02$. Furthermore, we prove that $T(a;U)$ is invariant under conformal transformations in an appropriate sense. The notion of a thick point is connected to the Liouville quantum gravity measure with parameter $\\gamma$ given formally by $\\Gamma(dz)=e^{\\sqrt{2\\pi}\\gamma F(z)}\\,dz$ considered by Duplantier and Sheffield.", "revisions": [ { "version": "v3", "updated": "2010-10-02T06:40:59.000Z" } ], "analyses": { "keywords": [ "thick point", "continuum gaussian free field", "liouville quantum gravity measure", "dirichlet inner product", "conformal transformations" ], "tags": [ "journal article" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "adsabs": "2009arXiv0902.3842H" } } }