We derive the transmission coefficient, T(ω), for grazing incidence of
crystals with spatial dispersion accounting for the excitation of multiple
modes with different wave vectors k for a given frequency ω. The
generalization of the Fresnel formulas contains the refraction indices of these
modes as determined by the dielectric function ϵ(ω,k). Near
frequencies ωe, where the group velocity vanishes, T(ω) depends
also on an additional parameter determined by the crystal microstructure. The
transmission T is significantly suppressed, if one of the excited modes is
decaying into the crystal. We derive these features microscopically for the
Josephson plasma resonance in layered superconductors.Comment: 4 pages, 2 figures, epl.cls style file, minor change