1987
DOI: 10.1016/0167-2738(87)90181-0
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Ionic transport in mixed sodium rubidium germanate glasses

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Cited by 15 publications
(6 citation statements)
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“…The superimposed plots in The temperature independence of the loss peaks may contradict the idea of a distribution of activation energies which has been suggested to explain the conductivity dispersion [58][59][60][61][62][63][64][65][66][67][68][69][70][71][72], however, the possibility exists that the distribution of activation energies may be frequency and thermally activated with the same d.c. activation energy. Alternatively, the possibility that the conductivity dispersion may be due to a second mechanism that contributes to the total conductivity and has a constant slope on a log frequency plot and is temperature independent.…”
Section: Conductivity Relaxationmentioning
confidence: 77%
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“…The superimposed plots in The temperature independence of the loss peaks may contradict the idea of a distribution of activation energies which has been suggested to explain the conductivity dispersion [58][59][60][61][62][63][64][65][66][67][68][69][70][71][72], however, the possibility exists that the distribution of activation energies may be frequency and thermally activated with the same d.c. activation energy. Alternatively, the possibility that the conductivity dispersion may be due to a second mechanism that contributes to the total conductivity and has a constant slope on a log frequency plot and is temperature independent.…”
Section: Conductivity Relaxationmentioning
confidence: 77%
“…This phenomenon has been widely reported for most alkali glasses in a similar composition range [57][58][59][60][61][62][63][64][65][66][67][68][69][70][71][72]. Martin and Angell have explained this phenomenon by suggesting that the ac tivation energy is a function of the amount of overlap between the potential energy wells of cation sites [57,65,70].…”
Section: DC Conductivitymentioning
confidence: 99%
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