Lp Solutions for Stochastic Evolution Equation with Nonlinear Potential
arXiv:1406.0970
Abstract
This article considers the stochastic partial differential equation \[ \left\{ \begin{array}{l} u_t = \frac{1}{2} u_{xx} + u^γξu(0,.) = u_0 \end{array}\right. \] \noindent where is a space / time white noise Gaussian random field, and is a non-negative initial condition independent of satisfying \[ u_0 \geq 0, \qquad \lim_{n \rightarrow +\infty} \mathbb{E} \left [ \left (\int_{\mathbb{S}^1} u_0 (x)\wedge n dx \right)^2 \right ] = \mathbb{E} \left [ \left (\int_{\mathbb{S}^1} u_0 (x) dx \right)^2 \right ]< +\infty.\] \noindent The {\em space} variable is with the identification . The definition of the stochastic term, taken in the sense of Walsh, will be made clear in the article. The result is that there exists a unique non-negative solution such that for all , \[\mathbb{E} \left [ \left( \int_0^\infty \int_{\mathbb{S}^1} u(t,x)^{2γ} dx dt \right)^{α/ 2 } \right ] \leq C( α) < + \infty. \] \noindent where the constant arises in the Burkholder-Davis-Gundy inequality. The solution is also shown to satisfy \[ \mathbb{E} \left [ \int_0^T \left(\int_{\mathbb{S}^1} u (t,x)^p dx \right)^{α/ p} dt \right ] < +\infty \qquad \forall T < +\infty, \qquad p < +\infty, \qquad α\in \left (0, \frac{1}{2} \right ). \]
proof involved change of probability space - it was not proved that the limiting object satisfied the equation