Je. Masnik et al., THE COMPLEX MECHANICAL MODULUS AS A STRUCTURAL PROBE - THE CASE OF ALKALI BORATE LIQUIDS AND GLASSES, The Journal of chemical physics, 103(23), 1995, pp. 9907-9917
Brillouin light scattering has been used to determine the high-frequen
cy complex mechanical modulus of alkali berate liquids and glasses, as
a function of the temperature. The temperature dependence of the comp
lex modulus can be described by an enhanced Maxwell model for linear v
iscoelastic systems. Accordingly, the module comprises relaxational co
mponents and a temperature dependent static modulus, which is determin
ed by the equilibrium volume fraction of kinetically arrested domains.
Application of this model to the Brillouin data indicates that the st
ructural relaxations in undercooled glass forming liquids occur via re
latively distinct mechanisms, each one becoming thermally activated wi
thin a different temperature range. The rate of degradation of the net
work structure increases with increasing alkali content, and is commen
surate of the fragility of the liquid. The structural features which a
re subject to a change in the context of a particular degradation mech
anism are released sequentially, i.e., relaxation, facilitated by the
rupture of a given network link, is required before other links of the
same type become affected by thermal motion. Mechanisms that are acti
vated at high temperatures involve the diffusional displacements of va
rious atomic species. Immediately above T-g, however, structural relax
ations are characterized by the dominance of the bulk viscosity over t
he shear viscosity, and by positive values of the imaginary part of th
e complex poison ratio. This indicates that, to a significant degree,
compressive deformations and head-on collisions between structural moi
eties are involved in the structural relaxations at these low temperat
ures. It is surmised that the deformation of boroxol rings, where a bo
ron moves out of the BO3 plane to exchange one of its oxygen neighbors
, is underlying to this relaxation mechanism, which results in an incr
ease of the average network ring size. (C) 1995 American Institute of
Physics.