The objective of this work is to investigate how the anisotropy of the inte
raction between dipole-active vibrations of a crystal lattice and infrared
electromagnetic waves is manifested in the spontaneous parametric light sca
ttering spectra of polaritons (Raman scattering by small angles). The case
where scattering occurs by extraordinarily polarized polaritons-quasipartic
les formed as a result of the coupling of the wave polarized in the symmetr
y plane of a biaxial crystal simultaneously with two phonons possessing ort
hogonal dipolar moments-is studied. A series of spectra of equilibrium fluc
tuations of the electromagnetic (infrared) field, each of which represents
an intensity distribution in frequency-wave number coordinates for a fixed
direction of the wave vector, are constructed on the basis of a scattering
model that takes account of the tensor character of the permittivity and th
e quadratic and cubic susceptibilities of the crystal. Analysis of the comp
uted spectra identified the basic laws and dependences which are determined
by the anisotropy of the electromagnetic susceptibilities of various order
s and made it possible to explain previous experimental results which canno
t be interpreted on the basis of the generally accepted model of transverse
ly polarized polaritons. A method is proposed for determining the contribut
ions of the dipole-active vibrations of the crystal lattice to the permitti
vity and the quadratic and cubic susceptibilities, as well as the absorptio
n of the material from the spectra of the extraordinarily polarized polarit
ons. (C) 2000 MAIK "Nauka/Interperiodica".