Oxygen Vacancy Formation and Migration within the Antiphase Boundaries in Lanthanum Scandate-Based Oxides: Computational Study

The atomic structure of antiphase boundaries in Sr-doped lanthanum scandate (La_1−xSr_xScO_3−δ) perovskite, promising as the proton conductor, was modelled by means of DFT method. Two structural types of interfaces formed by structural octahedral coupling were constructed: edge- and face-shared. The energetic stability of these two interfaces was investigated. The mechanisms of oxygen vacancy formation and migration in both types of interfaces were modelled. It was shown that both interfaces are structurally stable and facilitate oxygen ionic migration. Oxygen vacancy formation energy in interfaces is lower than that in the regular structure, which favours the oxygen vacancy segregation within such interfaces. The calculated energy profile suggests that both types of interfaces are advantageous for oxygen ion migration in the material.

Preparation, structure, and reactivity of Ge-containing heterometallic cube derivatives of [M(3)E(4)(H2O)(9)](4+) (M = Mo, W; E = S, Se)

Studies leading to the incorporation of Group 14 germanium into the incomplete cuboidal clusters [M(3)E(4)(H2O)(9)](4+) (M = Mo, W; E = S, Se) have been carried out. From the clusters [Mo(3)E(4)(H2O)(9)](4+), corner-shared double cubes [Mo(6)GeE(8)(H2O)(18)] are obtained with GeO, by heating with Ge powder at 90 degrees C, or by heating with GeO(2) in the presence of H(3)PO(2) as reductant at 90 degrees C, illustrating the dominance of the double cubes. The yellow-green single cube [Mo(3)GeS(4) (H2O)(12)](6+) is only obtained by controlled air oxidation of [Mo(6)GeS(8)(H2O)(18)](8+) over a period of approximately 4 days followed by Dowex purification. In the case of the trinuclear clusters [W(3)E(4)(H2O)(9)](4+), the single cubes [W(3)GeE(4)(H2O)(12)](6+) are dominant and prepared by the reactions with GeO, or GeO(2)/H(3)PO(2). Conversion of [W(3)GeE(4)(H2O)(12)](6+) to the corresponding double cubes is achieved by reductive addition with BH(4)(-) in the presence of a further equivalent of [W(3)E(4)(H2O)(9)](4+). The crystal structures (pts(-) = p-toluene-sulfonate) of [Mo(6)GeS(8)(H2O)(18)](pts)(8).28H2O, (1); [W(6)GeS(8)(H2O)(18)](pts)(8).23H2O, (2); and [Mo(6)GeSe(8)(H2O)(18)](pts)(8).8H2O, (3); have been determined, of which (2) is the first structure of a W(6) double cube. The M-M bond lengths of approximately 2.7 A are consistent with metal-metal bonding, and the M-Ge of approximately 3.5 A corresponds to nonbonding separations. Of the Group 13-15 corner-shared double cubes from [Mo(3)S(4)(H2O)(9)](4+), [Mo(6)GeS(8)(H2O)(18)](8+) is the least reactive with [Co(dipic)(2)](-) as oxidant (0.077 M(-1) s(-1)), and [Mo(6)SnS(8)(H2O)(18)](8+) is next (14.9 M(-1) s(-1)). Both Ge and Sn (Group 14) have an even number of electrons, resulting in greater stability. In contrast, [W(6)GeS(8)(H2O)(18)](8+) is much more reactive (7.3 x 10(3) M(-1) s(-1)), and also reacts more rapidly with O(2).

Behavioral patterns of heterometallic cuboidal derivatives of [M3Q4(H2O)9]4+ (M = Mo, W; Q = S, Se)

This Account reports recent progress in the study of some approximately 20 heterometal derivatives of [Mo3S4(H2O)9]4+ with reference also to W and Se analogues. Single cubes (3:1) and corner-shared double cubes (6:1), as well as dimers of the 3:1 single cubes, are considered. A classification of the heterometals as subtypes A, B, and C is introduced.