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Brownian motion and thermal capacity

Abstract

Let WW denote dd-dimensional Brownian motion. We find an explicit formula for the essential supremum of Hausdorff dimension of W(E)FW(E)\cap F, where E(0,)E\subset(0,\infty) and FRdF\subset \mathbf {R}^d are arbitrary nonrandom compact sets. Our formula is related intimately to the thermal capacity of Watson [Proc. Lond. Math. Soc. (3) 37 (1978) 342-362]. We prove also that when d2d\ge2, our formula can be described in terms of the Hausdorff dimension of E×FE\times F, where E×FE\times F is viewed as a subspace of space time.Comment: Published in at http://dx.doi.org/10.1214/14-AOP910 the Annals of Probability (http://www.imstat.org/aop/) by the Institute of Mathematical Statistics (http://www.imstat.org

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