The Boson peak in the Raman spectra of glasses is an ubiquitous feature. We
show that doping a series of fluoride, tellurite and sulfide glass composi
tions with rare-earth ions, such as Pr3+, Dy3+, Nd3+, Ce3+, at concentratio
ns between 1000 and 10,000 ppm, increases the amplitude of the Boson peak a
s compared to the respective undoped glasses. Further addition of rare-eart
h ions results in saturation and even reduction of the Boson peak ascribed
to clustering of dopants and/or devitrification of glass host. Prolonged ir
radiation of photorefractive sulfide glasses with near-bandgap laser light
also results in an increase of the Boson peak. A model is suggested for cha
nges in the intensity and position of the Boson peak with glass composition
, doping level, and after prolonged irradiation of photorefractive glasses.
We propose that the presence of non-bridging anion atoms, such as F, O or
S, (or anion atoms having strained bonds with increased polarizability), de
termines the Boson peak, as well as the solubility of rare-earth ions in gl
asses. (C) 1999 Elsevier Science B.V. All rights reserved.