Abstract
In the transition from the normal (n) to the superconducing (s) state the creep rate of metals increases, while with deformation at constant strain rate a relaxation of the flow stress ensues. In a model developed to account for these and allied observations, phonons, emitted (n→s) or absorbed (s→n) in pairing and depairing respectively in the process of the dissolution of filamentary forms of intermediate phase retained at dislocations to temperatures somewhat below and above T c, induce transient changes in the rates of thermal activation of the creep and relaxation. Pairing (n→s), as well as relaxation of the Cooper pair density (s→n) in the core regions of edge dislocations, is linked in the model to the occurrence of local thermal spikes. Their magnitudes are taken to be linear in the Ginzburg-Landau pair-breaking function α(T) assigned to gradients in the BCS gap-parameter at the centres of the dislocations. On introducing α/k into the equations of logarithmic creep and stress relaxation as measure of the temperature changes associated with the transients, available experimental results are well accounted for.