Nature of the boson peak in Raman spectra of sodium berate glass systems: influence of structural and chemical fluctuations and intermolecular interactions
Av. Baranov et al., Nature of the boson peak in Raman spectra of sodium berate glass systems: influence of structural and chemical fluctuations and intermolecular interactions, J RAMAN SP, 31(8-9), 2000, pp. 819-825
The nature of the boson peak in the low-wavenumber Raman spectra of (Na2O)(
x)-(B2O3)(1-x) glasses is analyzed to be a manifestation of intermolecular
interactions within regions of inhomogeneity, which are inherent to all gla
sses. The wavenumber of the boson peak satisfies the modified Szigeti and O
delevskii equation, previously successfully applied to studies of intermole
cular vibrations in organic liquids and their mixtures. This allows one to
conclude that the boson peak is connected with intermolecular interactions
of structural groups, which are not bound in a glass-forming network, but f
orm regions of structural and chemical inhomogeneities. The existence of su
ch regions in alkali metal berate glasses and their high concentration were
previously confirmed by small-angle x-ray scattering data. Thus intermolec
ular interactions can be described by a soft potential, It has been also fo
und that the absolute intensity of the boson peak substantially decreases w
ith an increase in the modifier concentration in accordance with the specif
ic heat and the thermal phonon conductivity behavior as well as the theoret
ical expectations for glasses with increasing fragility. However, this decr
ease does not have a monotonic character but exhibits a slight bump at x =
0.2. Such a concentration behavior is connected with a decrease in the free
volume in the vicinity of this concentration and a suppression of the rela
xation processes in favor of vibrational modes, which begin to contribute t
o the boson peak. Copyright (C) 2000 John Wiley & Sons, Ltd.