The temperature dependence of the dc conductivity {σ} of most glass-forming and crystalline ionic conductors is Arrhenius with constant activation energy, E_σ, at sufficiently low temperatures or conductivity levels. However, {σ} becomes non-Arrhenius at high temperatures or conductivity levels. We have found that the product, βE_σ, of the Kohlrausch stretching exponent for the conductivity relaxation, β, and the dc conductivity activation energy in the Arrhenius regime is approximately the same as the high temperature apparent activation energy, Eₐ, of σ at the temperature where {σ} reaches the high level of 1Ω^-1cm^-1 and the conductivity relaxation time τ_σ is of the order of 1 psec.
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Ngai et al. (1998) studied this question.
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