The propagation of a plane electromagnetic (TE) wave into a plane stratified medium in which the ionization density varies as exp (

) is investigated. The solution of the wave equation appears as a combination of Bessel functions of imaginary order and complex argument, but the magnitude of the reflection coefficient (taken at

) is given by the simple expression exp

, where

is the angle of incidence,

is the free-space wavelength and (

) is the ratio of electron collision frequency to the frequency of the field. In general, the field components must be obtained from a complex series, but at depths beyond the critical density asymptotic forms are given which display the rapid decay of the evanescent field in terms of elementary functions.