On the spatial dynamics of the solution to the stochastic heat equation

preprint2013arXivOpen access

Abstract

We consider the solution of ∂tu=∂x2u+∂x∂tB, (x,t)∈R×(0,∞)\partial_t u=\partial_x^2 u+\partial_x\partial_t B,\,(x,t)\in R\times(0,\infty), subject to u(x,0)=0, x∈Ru(x,0)=0,\,x\in R, where BB is a Brownian sheet. We show that uu also satisfies ∂x2u+[ (−∂t2)1/2+2∂x(−∂t2)1/4 ] ua=∂x∂tB~\partial_x^2 u +[\,(-\partial_t^2)^{1/2}+\sqrt{2}\partial_x(-\partial_t^2)^{1/4}\,]\,u^a= \partial_x\partial_t{\tilde B} in R×(0,∞)R\times(0,\infty) where uau^a stands for the extension of u(x,t)u(x,t) to (x,t)∈R2(x,t)\in R^2 which is antisymmetric in tt and B~\tilde{B} is another Brownian sheet. The new SPDE allows us to prove the strong Markov property of the pair (u,∂xu)(u,\partial_x u) when seen as a process indexed by x≥x0x\ge x_0, x0x_0 fixed, taking values in a state space of functions in tt. The method of proof is based on enlargement of filtration and we discuss how our method could be applied to other quasi-linear SPDEs.

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