Non-linear Rough Heat Equations

Abstract

This article is devoted to define and solve an evolution equation of the form $dy_t=Δy_t dt+ dX_t(y_t)$, where $Δ$ stands for the Laplace operator on a space of the form $L^p(\mathbb{R}^n)$, and $X$ is a finite dimensional noisy nonlinearity whose typical form is given by $X_t(φ)=\sum_{i=1}^N x^{i}_t f_i(φ)$, where each $x=(x^{(1)},...,x^{(N)})$ is a $γ$-Hölder function generating a rough path and each $f_i$ is a smooth enough function defined on $L^p(\mathbb{R}^n)$. The generalization of the usual rough path theory allowing to cope with such kind of systems is carefully constructed.