Structures of ordered tungsten- or molybdenum-containing quaternary perovskite oxides

• Published in: Journal of solid state chemistry 2012-01, Vol.185, p.107-116
• Main Authors: Day, Bradley E., Bley, Nicholas D., Jones, Heather R., McCullough, Ryan M., Eng, Hank W., Porter, Spencer H., Woodward, Patrick M., Barnes, Paris W.
• Format: Article
• Language: English
• Subjects: Boundaries; CARBON; CARBON IONS; CATIONS; CHALCOGENIDES; CHARGED PARTICLES; COHERENT SCATTERING; Condensed matter: structure, mechanical and thermal properties; CRYSTAL LATTICES; CRYSTAL STRUCTURE; Crystal structure and symmetry; Crystalline state (including molecular motions in solids); Crystallization; CRYSTALLOGRAPHY; CUBIC LATTICES; DIAMONDS; DIFFRACTION; Distortion; Double perovskite; ELECTROMAGNETIC RADIATION; ELEMENTS; Exact sciences and technology; Inorganic compounds; INORGANIC, ORGANIC, PHYSICAL AND ANALYTICAL CHEMISTRY; IONIZING RADIATIONS; IONS; METALS; MINERALS; MOLYBDENUM; MOLYBDENUM IONS; MONOCLINIC LATTICES; NEUTRON DIFFRACTION; Neutron diffraction and scattering; Neutron powder diffraction; NONMETALS; OXIDE MINERALS; OXIDES; OXYGEN COMPOUNDS; PEROVSKITE; PEROVSKITES; Physics; Quaternary perovskite; RADIATIONS; REFRACTORY METALS; SCATTERING; Single-crystal and powder diffraction; SPACE GROUPS; STRONTIUM IONS; Structure of solids and liquids; crystallography; Structure of specific crystalline solids; Symmetry; SYMMETRY GROUPS; TETRAGONAL LATTICES; Theory of crystal structure, crystal symmetry; calculations and modeling; TOLERANCE; Tolerances; TRANSITION ELEMENTS; TRIGONAL LATTICES; TUNGSTEN; TUNGSTEN IONS; X RADIATION; X-RAY DIFFRACTION; X-ray powder diffraction
• ISSN: 0022-4596; 1095-726X
• DOI: 10.1016/j.jssc.2011.11.007

The room temperature crystal structures of six A2MMoO6 and A2MWO6 ordered double perovskites were determined from X-ray and neutron powder diffraction data. Ba2MgWO6 and Ba2CaMoO6 both adopt cubic symmetry (space group Fm3̄m, tilt system a0a0a0). Ba2CaWO6 has nearly the same tolerance factor (t=0.972) as Ba2CaMoO6 (t=0.974), yet it surprisingly crystallizes with I4/m symmetry indicative of out-of-phase rotations of the MO6 octahedra about the c-axis (a0a0c−). Sr2ZnMoO6 (t=0.979) also adopts I4/m symmetry; whereas, Sr2ZnWO6 (t=0.976) crystallizes with monoclinic symmetry (P21/n) with out-of-phase octahedral tilting distortions about the a- and b-axes, and in-phase tilting about the c-axis (a−a−c+). Ca2CaWO6 (t=0.867) also has P21/n symmetry with large tilting distortions about all three crystallographic axes and distorted CaO6 octahedra. Analysis of 93 double perovskites and their crystal structures showed that while the type and magnitude of the octahedral tilting distortions are controlled primarily by the tolerance factor, the identity of the A-cation acts as the secondary structure directing factor. When A=Ba2+ the boundary between cubic and tetragonal symmetries falls near t=0.97, whereas when A=Sr2+ this boundary falls somewhere between t=1.018 and t=0.992. A survey of the tolerance factor of 41Mo/W- and 52Nb/Ta-containing quaternary perovskites plotted as a function of the difference between the two six-coordinate M-cation ionic radii. Compounds with cubic symmetry are represented by diamonds, those with tetragonal symmetry are represented by squares, those with I2/m monoclinic symmetry are represented by ×, and those with P21/n monoclinic symmetry are represented by triangles. White symbols represent compositions where A=Ba2+, gray symbols represent compositions where A=Sr2+, and black symbols represent where A=Ca2+. The filled circle represents rhombohedral Ba2BiTaO6 (t=0.961; space group—R3̄; tilt system—a−a−a−). References for the compounds included in this figure are listed in the Supporting Information File.▪ ► Reports the structures of six double perovskites containing either Mo6+ or W6+. ► Compounds with similar tolerance factors (t) exhibited different symmetries. ► This effect was observed in Sr2ZnMO6 and Ba2CaMO6 (M=Mo or W). ► Contains a structural survey of 93 double perovskites. ► Octahedral tilting distortions are controlled by t and the nature of the A-cation.