Abstract

The temperature dependence of the dc conductivity \ensuremath{\sigma} of most glass-forming and crystalline ionic conductors is Arrhenius with constant activation energy, ${E}_{\ensuremath{\sigma}}$, at sufficiently low temperatures or conductivity levels. However, \ensuremath{\sigma} becomes non-Arrhenius at high temperatures or conductivity levels. We have found that the product, $\ensuremath{\beta}{E}_{\ensuremath{\sigma}}$, of the Kohlrausch stretching exponent for the conductivity relaxation, $\ensuremath{\beta}$, and the dc conductivity activation energy in the Arrhenius regime is approximately the same as the high temperature apparent activation energy, ${E}_{a}$, of $\ensuremath{\sigma}$ at the temperature where \ensuremath{\sigma} reaches the high level of $1{\ensuremath{\Omega}}^{\ensuremath{-}1}{\mathrm{cm}}^{\ensuremath{-}1}$ and the conductivity relaxation time ${\ensuremath{\tau}}_{\ensuremath{\sigma}}$ is of the order of 1 psec.

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