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9.4 Super-Stoichiometric AB 5+x Alloys  259

                  400
                  350                          LaNi 3.85-x Co .75 Mn .4 Al x
                  300
                Capacity, Q, mAh/g  200  x = 0.3
                  250

                  150
                                        x = 0.2
                  100
                  50                    x = 0.1
                                        x = 0.0
                   0
                  -50
                         0     25    50     75    100   125    150
                                          Cycles
               Figure 9.15  Charge capacity, Q, vs charge–discharge cycles
               for LaNi 3.85−x Co .75 Mn .4 Al x electrodes [43].

               Table 9.7  Effect of Al in LaNi 3.85−x Co .75 Mn .4 Al x electrodes [43].
                          3
                                      −1
               x Value  V H ( ˚ A )  Q max (mAh g )  n,H atoms  % ∆V/V  Corrosion
                                           per unit cell      (wt%/cycle)
               0.2     3.01       314        4.98     16.66    0.1274
               0.3     2.99       330        5.18     17.33    0.1394
               0.1     3.01       327        5.22     17.58    0.2905
               0.0     3.20       353        5.66     20.39    0.4079
               0.0     3.35       366        5.88     22.30    0.4126



               9.4
               Super-Stoichiometric AB 5+x Alloys

               Notten et al. [51, 52] reported that the electrochemical cycling stability can be
               improved dramatically when using nonstoichiometric La(NiCu) 5+x alloys. They
               attributed such improvement to an alteration of the crystal structure in which
               the excess of B-type atoms is accommodated in the AB 5 lattice by the occupation
               of empty A sites (La) with dumbbell pairs of Ni atoms oriented along the c-axis,
               although the hexagonal P6/mmm space group is preserved.
                Recently Vogt et al. have shown that the structure of La .9 Ni 4.54 Sn .32 (a stoi-
               chiometry of AB 5.40 when La is normalized) also compensates for La deficiency
               by also inserting Ni dumbbells in empty A sites [53]. A representation of the
               La(Ni, Sn) 5+x lattice is shown in Figure 9.19. Here too the presence of Ni dumb-
               bells greatly improves the cycle life compared to two stoichiometric alloys as
               illustrated in Figure 9.20. Indeed it is remarkable that the super-stoichometric alloy,
               LaNi 4.84 Sn 0.32, performs better than the simulated commercial alloy containing Co.
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