The disorder-induced, low-wavenumber Raman scattering from glasses is
ascribed to the fluctuations of the elastooptic tensor (electrical dis
order) and of the local strain from its smooth envelope (mechanical di
sorder). Phenomenological models of first-order Raman scattering, whic
h are able to interpret (at least partially) the salient experimental
features, i.e. the Boson peak, the wavenumber dependence of the light-
vibration coupling coefficient and the depolarization ratio, are summa
rized and compared. The models considered are Martin and Brenig's mode
l, the non-continuous glass structure model and the soft potential mod
el. Results obtained from numerical simulations on model systems consi
sting of simple disordered structures are discussed.