A schematic model is proposed for understanding the boson peak as a consequ
ence of the coupling between slowly decaying density fluctuations and the t
ransverse sound modes th;lt develop in the amorphous solid. The present ana
lysis demonstrates that the nature of the dynamics of defect densities in t
he disordered system plays a crucial role for the appearance of the peak. W
e compare the results for the dynamic structure factor with the scattering
data of Sokolov et al.. [J. Non-Cryst. Solids 172-174. 138 (1994)]. With th
e relaxation time for the defects becoming longer which is the case more ap
propriate for the strong glasses as compared to the fragile glasses where s
tructural degradation occurs more easily, the boson peak become more pronou
nced.