Exact formulation of Huygens' principle in terms of generalized spatiotemporal-dipole secondary sources

TL;DR

This paper derives an exact formulation of Huygens' principle using generalized spatiotemporal dipole sources, allowing precise wave cancellation and a geometrical-optical explanation of wave behavior.

Contribution

It introduces a generalized spatiotemporal dipole model that enables exact wave matching and cancellation, extending traditional Huygens' principle to more flexible and precise wave source representations.

Findings

GSTD sources can cancel waves at specific angles and distances.

The formulation matches Kirchhoff's integral theorem exactly.

Provides a geometrical-optical explanation for wave suppression phenomena.

Abstract

A "spatiotemporal dipole" wave source, as defined by D.A.B. Miller (1991), differs from an ordinary ("spatial") dipole source in that the inverted monopole is delayed relative to the uninverted monopole, the delay being equal to the propagation time from one monopole to the other. A "generalized" spatiotemporal dipole (GSTD), as defined here, is generalized in two ways: first, the delay may be smaller in absolute value (but not larger) than the propagation time, so that the radiated waves cancel at a certain angle from the axis of the dipole; second, one monopole may be attenuated relative to the other, so that the cancellation is exact at a finite distance - on a circle coaxial with the dipole. I show that the Kirchhoff integral theorem, for a single monopole primary source, gives the same wave function as a certain distribution of GSTD secondary sources on the surface of integration. In the GSTDs, the "generalized" delay allows the surface of integration to be general (not necessarily a primary wavefront), whereas the attenuation allows an exact match of the wave function even in the near field of the primary source. At each point on the surface of integration, the circle of cancellation of the GSTD secondary source passes through the primary source, which therefore receives no backward secondary waves, while the direction of specular reflection of the primary wave passes through the same circle, giving a geometrical-optical explanation of the suppression of backward secondary waves at any field point.