Abstract
The jump rate k for atomic diffusion via the vacancy mechanism in crystals is evaluated by treating a jump as the result of a particular type of thermal fluctuation in a crystal. The occurrence rate of this fluctuation is found (a) using a dynamical method similar in content to that of Rice and Manley, and (b) using statistical mechanics directly as was done by Vineyard. If the jumps are effected only when the surrounding atoms take up one single distorted configuration (the first approach being limited to describing one configuration only) then both methods are exactly equivalent and give the same k (Sec. II)

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