Asymptotic expansions for the solution of a linear PDE with a multifrequency highly oscillatory potential
Rafał Perczyński, Antoni Augustynowicz
TL;DR
This work develops an analytic Modulated Fourier Expansion for linear PDEs with multifrequency highly oscillatory potentials by representing the solution as a convergent Neumann series in the Sobolev space $H^{2p}(\Omega)$. It derives a fully analytic computation of the expansion coefficients and a precise asymptotic expansion for the highly oscillatory multivariate integrals underlying each Neumann-term, under a nonresonance condition, and extends the framework to second-order time derivatives (wave/Klein–Gordon) equations. The authors provide error bounds of the form $\mathcal{O}(\omega^{-(r+1)})$ for a truncated expansion with parameter $r$, and demonstrate the approach via numerical experiments showing accuracy for practical $\omega$ and systems. The results enable long-time, high-frequency simulations without solving large differential systems, and point to extensions including Filon-type quadrature and more general oscillatory potentials.
Abstract
Highly oscillatory differential equations present significant challenges in numerical treatments. The Modulated Fourier Expansion (MFE), used as an ansatz, is a commonly employed tool as a numerical approximation method. In this article, the Modulated Fourier Expansion is analytically derived for a linear partial differential equation with a multifrequency highly oscillatory potential. The solution of the equation is expressed as a convergent Neumann series within the appropriate Sobolev space. The proposed approach enables, firstly, to derive a general formula for the error associated with the approximation of the solution by MFE, and secondly, to determine the coefficients for this expansion -- without the need to solve numerically the system of differential equations to find the coefficients of MFE. Numerical experiments illustrate the theoretical investigations.
