It is shown that the interaction between vibrational modes polarized parall
el and perpendicular to the layers in a strongly anisotropic layered crysta
l is very weak for frequencies above the van Hove frequency, which correspo
nds to a transition from closed isofrequency surfaces to surfaces which are
open in the weak-coupling direction. Such mode quasisplitting results in q
uasi-two-dimensional behavior of phonons polarized along layers and quasi-o
ne-dimensional behavior of phonons polarized in a direction perpendicular t
o the layers and localized near light or strongly coupled impurity atoms or
monolayers. (C) 2001 American Institute of Physics.