Jr. Macdonald, Comparison of the universal dynamic response power-law fitting model for conducting systems with superior alternative models, SOL ST ION, 133(1-2), 2000, pp. 79-97
For at least 5 years there has been considerable controversy concerning the
relative value of power-law and electric modulus formalism models for fitt
ing and interpreting dispersed frequency-response data for ionically conduc
ting glasses, melts, and other disordered solids. Conclusions of various au
thors have ranged from preferring one or the other to neither. Here, detail
ed complex-nonlinear-least-squares fitting of data for a trisilicate glass
with several different dispersion models leads to the conclusion that 'neit
her' of the above is the correct conclusion for an adequate analysis of bul
k-material behavior in this and other materials. The power-law model is non
physical, and the usual modulus formalism approach is faulty in two differe
nt ways. For the near-room-temperature data set analyzed here, it was found
that when electrode effects were included in a composite fitting model, th
ey contributed significantly to high-, but not low-frequency response. Thei
r presence may explain the increasing log-log slope of the real part of the
conductivity with increasing frequency found for many materials. The corre
cted modulus formalism approach, involving a Kohlrausch-Williams-Watts mode
l, the KWW1, was found to be the best of those used to represent bulk respo
nse. Contrary to common expectation, the original modulus formalism and KWW
1 models do not lead to stretched-exponential response in the time domain.
Best fitting required not only a model for bulk response but one for electr
ode response as well and necessarily also involved a separate fitting param
eter to account for high-frequency-limiting dipolar dielectric effects. (C)
2000 Elsevier Science B.V. All rights reserved.