The power-law frequency dependence of both the conductivity, {σ}({ω}), and permittivity, {ε}({ω}), of ion-conducting materials suggests that self-similar or scale-invariant behavior influences the transport of ions at high frequencies. Using an anomalous-diffusion model, we derive relevant power-law expressions for {σ}({ω}) and {ε}({ω}) and compare these with measurements performed on LiPO₃ glass. Superior fits to the measured data are obtained compared to the commonly used Kohlrausch-Williams-Watts (KWW) description of the electrical modulus, most particularly in the notorious high-frequency regime. Evaluation of our results in terms of an anomalous-diffusion model suggests the dominance of interaction-based constraints to diffusion.
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Sidebottom et al. (1995) studied this question.
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