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Analysis

This paper introduces a novel, positive approximation method for the parabolic Anderson model, leveraging the Feynman-Kac representation and random walks. The key contribution is an error analysis for the approximation, demonstrating a convergence rate that is nearly optimal, matching the Hölder continuity of the solution. This work is significant because it provides a quantitative framework for understanding the convergence of directed polymers to the parabolic Anderson model, a crucial connection in statistical physics.
Reference

The error in $L^p (Ω)$ norm is of order \[ O ig(h^{ rac{1}{2}[(2H + H_* - 1) \wedge 1] - ε}ig), \] where $h > 0$ is the step size in time (resp. $\sqrt{h}$ in space), and $ε> 0$ can be chosen arbitrarily small.