Weil Matthias, Stöger Berthold
Institute for Chemical Technologies and Analytics, Division of Structural Chemistry, Getreidemarkt 9/164-SC, A-1060 Vienna, Austria.
Acta Crystallogr B. 2010 Dec;66(Pt 6):603-14. doi: 10.1107/S0108768110040802. Epub 2010 Nov 17.
The structures of the 3d divalent transition-metal diarsenates M(2)As(2)O(7) (M = Mn, Co, Ni, Zn) can be considered as variants of the monoclinic (C2/m) thortveitite [Sc(2)Si(2)O(7)] structure type with a ≃ 6.7, b ≃ 8.5, c ≃ 4.7 Å, α ≃ 90, β ≃ 102, γ ≃ 90° and Z = 2. Co(2)As(2)O(7) and Ni(2)As(2)O(7) are dimorphic. Their high-temperature (β) polymorphs adopt the thortveitite aristotype structure in C2/m, whereas their low-temperature (α) polymorphs are hettotypes and crystallize with larger unit cells in the triclinic crystal system in space groups P\bar 1 and P1, respectively. Mn(2)As(2)O(7) undergoes no phase transition and likewise adopts the thortveitite structure type in C2/m. Zn(2)As(2)O(7) has an incommensurately modulated crystal structure [C2/m(α,0,γ)0s] with q = [0.3190 (1), 0, 0.3717 (1)] at ambient conditions and transforms reversibly to a commensurately modulated structure with Z = 12 (I2/c) below 273 K. The Zn phase resembles the structures and phase transitions of Cr(2)P(2)O(7). Besides descriptions of the low-temperature Co(2)As(2)O(7), Ni(2)As(2)O(7) and Zn(2)As(2)O(7) structures as five-, three- and sixfold superstructures of the thortveitite-type basic structure, the superspace approach can also be applied to descriptions of all the commensurate structures. In addition to the ternary M(2)As(2)O(7) phases, the quaternary phase (Ni,Co)(2)As(2)O(7) was prepared and structurally characterized. In contrast to the previously published crystal structure of the mineral petewilliamsite, which has the same idealized formula and has been described as a 15-fold superstructure of the thortveitite-type basic structure in space group C2, synthetic (Ni,Co)(2)As(2)O(7) can be considered as a solid solution adopting the α-Ni(2)As(2)O(7) structure type. Differences of the two structure models for (Ni,Co)(2)As(2)O(7) are discussed.
三维二价过渡金属二砷酸盐M₂As₂O₇(M = Mn、Co、Ni、Zn)的结构可被视为单斜晶系(C2/m)钪钇硅石[Sc₂Si₂O₇]结构类型的变体,其a ≃ 6.7 Å,b ≃ 8.5 Å,c ≃ 4.7 Å,α ≃ 90°,β ≃ 102°,γ ≃ 90°,Z = 2。Co₂As₂O₇和Ni₂As₂O₇具有二型性。它们的高温(β)多晶型物采用C2/m空间群中的钪钇硅石原型结构,而它们的低温(α)多晶型物是异质同晶型,分别在三斜晶系的P(\bar{1})和P1空间群中以更大的晶胞结晶。Mn₂As₂O₇不发生相变,同样采用C2/m空间群中的钪钇硅石结构类型。Zn₂As₂O₇在环境条件下具有非公度调制晶体结构[C2/m(α,0,γ)0s],q = [0.3190 (1), 0, 0.3717 (1)],并在273 K以下可逆地转变为Z = 12(I2/c)的公度调制结构。Zn相类似于Cr₂P₂O₇的结构和相变。除了将低温Co₂As₂O₇、Ni₂As₂O₇和Zn₂As₂O₇结构描述为钪钇硅石型基本结构的五重、三重和六重超结构外,超空间方法也可用于描述所有公度结构。除了三元M₂As₂O₇相外,还制备了四元相(Ni,Co)₂As₂O₇并对其进行了结构表征。与先前发表的具有相同理想化化学式且被描述为C2空间群中钪钇硅石型基本结构的15重超结构的矿物彼得威廉斯石的晶体结构不同,合成的(Ni,Co)₂As₂O₇可被视为采用α-Ni₂As₂O₇结构类型的固溶体。讨论了(Ni,Co)₂As₂O₇的两种结构模型的差异。