The Vogel-Fulcher equation (and percolation approach) predicts an infinite
resistivity below the "ideal" glassification point T-0 (correspondingly- pe
rcolation threshold). However, the ions still preserve a noticeable mobilit
y within the real glasses even below To. T-0 model the finite resistivity i
n glass a resistance R-max of a broken bond is introduced. The ratio of R-m
ax/R-min in real glasses is about 10(14) and 1/R-max might be identified wi
th a probability of tunnelling process. The comparison of calculations' res
ult (with R-max/R-min = 10(7) or 10(9)) with our data on CKN is encouraging
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