(This is a continuation of my “history of invisibility physics” series of posts. The earlier posts are: Part I, Part II, Part III.)
Up through the late 1940s, it seems that the only type of invisibility that authors were considering were “radiationless orbits”: motions of charged particles of extended size which in principle could accelerate without emitting radiation. These are not invisible objects per se, but rather objects that should produce radiation according to conventional wisdom but in fact do not.
A truly invisible object would be one which does not scatter any radiation incident upon it; that is, light which shines on the object is not reflected or absorbed, but instead is transmitted in such a way that it appears to the outside observer as if there were no object present. But are such invisible objects even possible?
In 1956, a paper appeared in the Journal of Applied Physics which provided at least a partial answer to this question. In their article, “Reflectionless transmission through dielectrics and scattering potentials,” Irvin Kay and Harry Moses demonstrated theoretically that one could construct stratified media that perfectly transmit waves of a given frequency, regardless of the direction of incidence of the illuminating wave. Light shining on their theoretical media would be completely transmitted, with no reflected light!




