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Thick Points of the Gaussian Free Field
Probability| Speaker: | Jason Miller, Stanford University |
| Location: | 2112 MSB |
| Start time: | Wed, Oct 22 2008, 4:10PM |
Description
Let $U \subseteq \C$ 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 $T_U(a)$ 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 $\sqrt{a/\pi} \log \tfrac{1}{r}$ as $r
\to 0$. We show that for each $0 \leq a \leq 2$ the Hausdorff
dimension of $T_U(a)$ is almost surely $2-a$ and that $T_U(a)$ is
invariant under conformal transformations in an appropriate sense.
The notion of a thick point is connected to the Liouville quantum
gravity measure considered by Duplantier and Sheffield.
Joint work with Xiaoyu Hu and Yuval Peres
