Abstract

A new angle of incidence of significance, when considering the reflection of electromagnetic waves at interfaces between transparent media, is defined. At this angle, denoted by φe, the reflection coefficient of parallel-polarized radiation is equal in magnitude and opposite in sign to the reflection coefficient at normal incidence. No similar angle exists for the perpendicular polarization. If e is the relative dielectric constant, i.e., the ratio of the dielectric constant of the medium of refraction to that of the medium of incidence, we find that tan φe=(e2+e)1/2. Measurement of φe, by equalization of the absolute (intensity) reflectances at normal and oblique incidence, allows e to be determined using the inverse relation e=(tan2φe+1/4)1/2−1/2.

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