Scattering on the line via singular approximation

TL;DR

This paper develops a new framework for analyzing scattering in one-dimensional wave equations with highly singular coefficients, introducing the generalized reflection coefficient and related algorithms for forward and inverse scattering.

Contribution

It introduces the generalized reflection coefficient and a harmonic exponential operator, enabling analysis of more singular coefficients than previous theories and providing explicit formulas and algorithms.

Findings

New explicit formulas for scattering with singular coefficients

Effective nonlinear algorithms akin to FFT for scattering problems

Elementary scattering relation at or below the critical impedance threshold

Abstract

Motivated by applications to acoustic imaging, the present work establishes a framework to analyze scattering for the one-dimensional wave, Helmholtz, Schr\"odinger and Riccati equations that allows for coefficients which are more singular than can be accommodated by previous theory. In place of the standard scattering matrix or the Weyl-Titchmarsh $m$-function, the analysis centres on a new object, the generalized reflection coefficient, which maps frequency (or the spectral parameter) to automorphisms of the Poincar\'e disk. Purely singular versions of the generalized reflection coefficient, which are amenable to direct analysis, serve to approximate the general case. Orthogonal polynomials on both the unit circle and unit disk play a key technical role, as does an exotic Riemannian structure on PSL$(2,\mathbb{R})$. A central role is also played by the newly-defined harmonic exponential operator, introduced to mediate between impedance (or index of refraction) and the reflection coefficient. The approach leads to new, explicit formulas and effective algorithms for both forward and inverse scattering. The algorithms may be viewed as nonlinear analogues of the FFT. In addition, the scattering relation is shown to be elementary in a precise sense at or below the critical threshold of continuous impedance. For discontinuous impedance, however, the reflection coefficient ceases to decay at infinity, the classical trace formula breaks down, and the scattering relation is complicated by the emergence of almost periodic structure.