Mg is an attractive hydrogen storage material not only because of its high gravimetric and volumetric hydrogen capacities but also because of it low material costs. However, the hydride of MgH 2 is too stable to release hydrogen under moderate conditions. We demonstrate that the formation of nanometer-sized clusters of Mg reduces the stability of MgH 2 by the interface energy effect in the immiscible Mg−Ti system. Ti-rich Mg x Ti 1−x (x < 0.5) thin films deposited by magnetron sputtering have a hexagonal close packed (HCP) structure, which forms a face-centered cubic (FCC) hydride phase upon hydrogenation. Positron Doppler broadening depth profiling demonstrates that after hydrogenation, nanometer-sized MgH 2 clusters are formed which are coherently embedded in an FCC TiH 2 matrix. The P (pressure)−T (optical transmission) isotherms measured by hydrogenography show that these MgH 2 clusters are destabilized. This indicates that the formation of nanometer-sized Mg allows for the development of a lightweight and cheap hydrogen storage material with a lower desorption temperature.
■ INTRODUCTIONMg is one of the typical lightweight metals with a density of 1.74 g cm −3 , which is much less than that of many transition and rare earth metals. 1 Mg has a hexagonal close-packed (HCP) structure, and that forms the hydride phase MgH 2 by hydrogenation. MgH 2 has a rutile-type body-centered tetragonal (BCT) structure (α-MgH 2 ) at moderate temperatures and pressures. 2,3 The gravimetric hydrogen capacity is 7.6 mass %, which is higher than most metal hydrides. The volumetric hydrogen capacity of 109 g-H 2 l −1 corresponds to 2.9 times the gaseous hydrogen concentration under a pressure of 70 MPa and 1.6 times the one of liquid hydrogen at 20 K. 4 Mg is one of the most attractive hydrogen storage materials not only because of the high capacity but also the low material costs. However, MgH 2 is too stable to desorb hydrogen at moderate temperatures and pressures and thus unsuited for practical applications. The enthalpy for hydride formation is −75 kJ mol −1 -H 2 , 2,3 which corresponds to a dehydrogenation temperature of around 550 K under a hydrogen pressure of 0.1 MPa. Furthermore, the slow reaction kinetics for hydrogenation and dehydrogenation is a disadvantage for using it as hydrogen storage material. The diffusion of hydrogen in both Mg and MgH 2 has been studied, 2,5,6 and the activation energy for hydrogen diffusion in MgH 2 of 140 kJ mol −1 is particularly high. 6 This value is around 2−5 times those in hydrides of LaNi 5 7 and V. 8 A possible way to destabilize MgH 2 and enhance the reaction kinetics is to reduce the size of Mg. It has been calculated that MgH 2 is destabilized by decreasing the size on a nanometer scale. 9−11 The destabilization is remarkable for a MgH 2 cluster with a diameter below 1.3 nm, corresponding to 19 Mg atoms or less. 11 On the basis of these calculations, the dehydrogenation temperature for a MgH 2 cluster of 0.9 nm would be more than 100 K lower than for bulk MgH 2 under a given hydr...