A theory of the low-frequency vibrational spectra in disordered system
s is proposed and is based on accounting for small statistical fluctua
tions of the sound velocity. Long-range quasilocalized sound excitatio
ns of a circular nature are predicted. A circular excitation is locali
zed during its lifetime inside an appropriate fluctuation that has the
form of a thin tube bent into a ring. The density of states of such e
xcitations estimated by the optimum fluctuation method depends exponen
tially on the frequency. The existence of a characteristic frequency i
s found at which the density of the quasilocalized states competes wit
h that of phonons, providing a kind of anomaly in the total density of
vibrational states. This frequency depends both on the correlation ra
dius of the disorder and its amplitude. The theory predicts qualitativ
ely a universal behavior of the density of vibrational states in vario
us disordered systems possessing medium-range order.