In order to determine the parameters of H motion in the cubic (C15-type͒ Laves phase ZrMo 2 , we have performed quasielastic neutron scattering measurements and nuclear-magnetic-resonance measurements of the proton spin-lattice relaxation rate on ZrMo 2 H x (0.3рxр1.0) in the temperature range 10-430 K. The diffusive motion of hydrogen in this system can be described in terms of two jump processes: the fast localized H motion within the hexagons formed by interstitial g (Zr 2 Mo 2 ) sites and the slower hopping from one hexagon to the other. The hopping rate l Ϫ1 of the faster process is found to be of the order of 10 10 s Ϫ1 at 300 K. The characteristic frequency d Ϫ1 of the slower process at the same temperature is about 6ϫ10 7 s Ϫ1
In order to study the mechanism and parameters of hydrogen diffusion in the cubic (C15-type) Laves phase YMn 2 , we have performed quasielastic neutron scattering measurements in YMn 2 H x (x = 0.4, 0.65 and 1.26) over the temperature range 30-395 K. It is found that the diffusive motion of hydrogen in this system can be described in terms of two jump processes: the fast localized H motion with the jump rate τ −1 l and the slower process with the rate τ −1 d associated with H jumps leading to long-range diffusion. The ratio τ d /τ l at room temperature is close to 10 2 . Our results suggest that the localized H motion in YMn 2 H x corresponds to back-and-forth jumps of hydrogen atoms within pairs of interstitial g (Y 2 Mn 2 ) sites. The parameters of the long-range diffusion of hydrogen in the samples with different H content are found to be close to each other. In the range 210-395 K, the temperature dependences of τ −1 d and the hydrogen diffusivity are reasonably described by the Arrhenius law with activation energies 0.18-0.22 eV.
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