Abstract
Most available data for diffusion of hydrogen isotopes in fcc metals show Arrhenius behavior with preexponential factors which exhibit the classical inverse-square-root mass dependence but with activation energies U which show the anomalous behavior UH>UD>UT. This behavior may be understood in terms of a quantum rate theory based on Gaussian wave-packet ensembles in which the stright-line Arrhenius behavior arises from the opposing effects of quantum statistics and tunneling.