Abstract
A derivation of the classical jump rate Γ for tracer diffusion aimed at a clear expression for the mass dependence of the frequency factor ν¯ is presented. The derivation is effected without using the usual collective normal coordinates which usually combine the masses in a complicated way. ν¯ depends explicitly on the mass of the surrounding host atoms (as well as on the tracer-atom mass) if these atoms must move to new equilibrium positions after the jump. ν¯ then has much the same form as suggested for a many-atom jump process. The contribution of the surrounding atoms is reduced (increased) for light (heavy) tracer atoms.

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