# Feynman-Kac representation for the parabolic Anderson model driven by   fractional noise

**Authors:** Kamran Kalbasi, Thomas S. Mountford

arXiv: 1706.09050 · 2017-06-29

## TL;DR

This paper establishes a Feynman-Kac representation for the parabolic Anderson model driven by fractional noise with any Hurst parameter, using Stratonovich integration and Gaussian approximations.

## Contribution

It introduces a unified approach to represent solutions of the fractional noise-driven parabolic Anderson model via Feynman-Kac formula for all Hurst parameters.

## Key findings

- Feynman-Kac representation is valid for the fractional noise case.
- The approach works uniformly for all Hurst parameters in (0,1).
- Provides a rigorous solution framework for fractional noise-driven PDEs.

## Abstract

We consider the parabolic Anderson model driven by fractional noise: $$ \frac{\partial}{\partial t}u(t,x)= \kappa \boldsymbol{\Delta} u(t,x)+ u(t,x)\frac{\partial}{\partial t}W(t,x) \qquad x\in\mathbb{Z}^d\;,\; t\geq 0\,, $$ where $\kappa>0$ is a diffusion constant, $\boldsymbol{\Delta}$ is the discrete Laplacian defined by $\boldsymbol{\Delta} f(x)= \frac{1}{2d}\sum_{|y-x|=1}\bigl(f(y)-f(x)\bigr)$, and $\{W(t,x)\;;\;t\geq0\}_{x \in \mathbb{Z}^d}$ is a family of independent fractional Brownian motions with Hurst parameter $H\in(0,1)$, indexed by $\mathbb{Z}^d$. We make sense of this equation via a Stratonovich integration obtained by approximating the fractional Brownian motions with a family of Gaussian processes possessing absolutely continuous sample paths. We prove that the Feynman-Kac representation \begin{equation} u(t,x)=\mathbb{E}^x\Bigl[u_o(X(t))\exp \int_0^t W\bigl(\mathrm{d}s, X(t-s)\bigr)\Bigr]\,, \end{equation} is a mild solution to this problem. Here $u_o(y)$ is the initial value at site $y\in\mathbb{Z}^d$, $\{X(t)\;;\;t\geq0\}$ is a simple random walk with jump rate $\kappa$, started at $x \in \mathbb{Z}^d$ and independent of the family $\{W(t,x)\;;\;t\geq0\}_{x\in\mathbb{Z}^d}$ and $\mathbb{E}^x$ is expectation with respect to this random walk. We give a unified argument that works for any Hurst parameter $H\in (0,1)$.

## Full text

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## References

14 references — full list in the complete paper: https://tomesphere.com/paper/1706.09050/full.md

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Source: https://tomesphere.com/paper/1706.09050