COMPOSITION DEPENDENT ELECTRICAL-CONDUCTIVITY OF ESS-THAN-OR-EQUAL-TO-Y-LESS-THAN-OR-EQUAL-TO-0.70, AL-TO-X-LESS-THAN-OR-EQUAL-TO-0.4(X)AG2O.P2O5]YAGI GLASSES IN THE RANGE 0.55)
A. Costantini et al., COMPOSITION DEPENDENT ELECTRICAL-CONDUCTIVITY OF ESS-THAN-OR-EQUAL-TO-Y-LESS-THAN-OR-EQUAL-TO-0.70, AL-TO-X-LESS-THAN-OR-EQUAL-TO-0.4(X)AG2O.P2O5]YAGI GLASSES IN THE RANGE 0.55), Physics and Chemistry of Glasses, 37(5), 1996, pp. 193-195
Glasses of the following general formula were prepared in order to inv
estigate their electrical and thermal properties: (1-y) [(1+x) Ag2O.P-
2 O-5]yAgI, 0.55 less than or equal to y less than or equal to 0.70, 0
less than or equal to x less than or equal to 0.4. Experimental data
confirm that, as reported in the literature, the increase of the AgI c
ontent makes the electrical conductivity, sigma, increase and the glas
s transformation temperature T-g decrease. The increase of sigma is pr
imarily due to the decrease of the activation energy for conduction, E
(sigma). The results can be interpreted on the basis of the model repo
rted in the literature of a glass demixed in AgI microdomains and a ph
osphate matrix. They suggest that the Ag+ migration paths also involve
sites other than the ones near I- ions and that E(sigma) for the AgI
doped glasses can be considered an average of the values relative to t
he various phases present. As it happens in glasses poorer in AgI cont
ent, a linear relation is observed when the ratio E(sigma)/E(sigma ma)
of the activation energies of AgI doped, E(sigma) and undoped, E(sigm
a ma) glasses is plotted against the fraction of Ag+ ions introduced a
s Ag2O.