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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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H. R. Glyde (1969) studied this question.
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