“…We find that if the data are force-fitted to log Rw(&/T)l/" then To = 1.5 x 10" K for the film as deposited and To = 2.5 x lo9 K following bombardment. Using the model of Apsley and Hughes (1974) with a localization length of lo& the corresponding densities of neutral defects at the Fermi level are 6 x stateseV-' cm-3 for the pristine film and 3.5 x 10l6 stateseV-l cm-3 for bombarded material. Though conduction in these a-Te films appears to be via the same mechanism as for the group IV and V elements studied, the density of defects responsible is much lower in a-Te than in the other materials.…”