Inverse Wave Propagator

Éamon Lalor

Journal of Mathematical Physics · 1968 · 29 citations · 4 references

Concepts

TL;DR

The inverse diffraction problem seeks the field at z = 0 from measurements at z > 0, and Wolf and Shewell previously solved it using a singular kernel. This paper rigorously addresses the inverse diffraction problem. The authors employ an angular‑spectrum representation of the field, illustrating its effectiveness. They demonstrate that a suitable truncation eliminates the need for a singular kernel or generalized function theory.

Abstract

In a recent publication, Wolf and Shewell gave a formal solution to the inverse diffraction problem, i.e., to finding the field distribution in the plane z = 0 from the knowledge of the field in an arbitrary plane z = z1 > 0 in the half-space into which the field is propagated. The solution involved the use of a singular kernel. In the present paper the inverse diffraction problem is treated in a rigorous manner. Our method makes use of the representation of the field as an angular spectrum of plane waves and demonstrates the usefulness of this type of representation. It is shown that by the use of a suitable truncation procedure one may avoid the use of a singular kernel or the generalized function theory.

References

4