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               448                                                                                    Metal Hydrides










































                      FIGURE 3 Interstitial sites in (a) a Cu type structure (cubic closest packed structure, ccp) and (b) a cubic Laves
                      phase (MgCu 2 type, C15). (a) In a Cu-type arrangement of n metal atoms (large spheres), n octahedral (small filled
                      spheres), and 2n tetrahedral voids (small empty spheres) are found. The surroundings of one representative of each
                      is shown. (b) In a cubic Laves phase AM 2 (M 4 tetrahedra drawn out), three types of tetrahedral voids are available for
                      hydrogen: those surrounded by two A and two M, [A 2 M 2 ], by one A and three M, [AM 3 ], and those surrounded by M
                      only, [M 4 ]. For the sake of clarity only one representative of each type of interstice is shown with its surroundings.


                                                                                              −
               structure undergoes a reconstruction to a trigonal trihy-  lic conductivity in MH 2 (M e (H ) 2 ) and nonmetallic
                                                                                        3+ −
                                                                                  3+
                                                                                      −
               dride phase (HoD 3 type structure) on hydrogen uptake.  behavior in MH 3 (M (H ) 3 ) due to the presence or ab-
               The balance between attractive M–H and repulsive H–H  sence of itinerant electrons, respectively. Consequently,
               interactions determines which one of the two trihydride  approaching the maximum hydrogen content MH 3 leads
               structures will be more stable. As the atomic radius de-  to a metal–semiconductor transition. The accompanying
               creases along the lanthanide series and the void radius for  transition in the optical properties can be used to produce
               hydrogen occupation decreases as well, H–H repulsion  switchable mirrors (Fig. 4). The unusual feature of a de-
               becomes more important, favoring the trigonal over the  crease in the unit cell volume on hydrogen uptake from
               cubic structure for the heavier rare earths. In trihydrides  MH 2 to MH 2.4 and an enhanced sensitivity toward air for
               of the cubic CeD 3 type, the octahedrally coordinated  samples MH >2.2 points at an increasing saltlike charac-
               hydrogen atoms perform large anharmonic vibrations.  ter with increasing hydrogen content x in MH 2<x<3 .For
               This leads to a structural description in which those hy-  these intermediate compositions the octahedral holes are
               drogen positions are displaced by about 20 pm along the  only partially filled, i.e., H has got a partially disordered
               cell diagonal [111] cub away from the middle of the octa-  structure and an order–disorder transition occurs accom-
               hedral interstice. A similar displacement in the trigonal  panied by a tetragonal distortion. EuH 2 and YbH 2 are
               HoD 3 type structure is presumably due to H–H repulsion.  saltlike hydrides that adopt the PbCl 2 type structure as
               Both the dihydrides MH 2 and the trihydrides MH 3 exhibit  the corresponding dihydrides of Ca, Sr, and Ba. YbH 2
               considerable nonstoichiometry ranges. In both the metal  may take up further hydrogen to form the mixed-valent
               adopts the oxidation state of +III, causing good metal-  YbH 2.4 .
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