The crystal structure of calcium metaarsenate, CaAs<sub>2</sub>O<sub>6</sub>

Stefanidis, T.; Nord, Anders G.; Kierkegaard, Peder

doi:10.1524/zkri.1985.173.3-4.313

Cited by 7 publications

(7 citation statements)

References 7 publications

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“…For the interfacial distance parallel to c, we find values of 2.11 (1)-2.12 (1) A, whereas a regular octahedron wouldgive (2/31/2) times the Sb--O distance, i.e. Stefanidis, Nord & Kierkegaard (1985) reinvestigated CaAs206, using data to 20 = 86 ° photometered from two Guinier photographs taken with Cu Ka radiation. The triangular faces normal to c are also not perfectly staggered at 60 ° angles, but are found at 2arctan[2(31/2)(~ -x)] = 47.5 (3), 45.2 (5) and 42.6 (5) ° for the Ca, Sr and Ba cases, respectively.…”

Section: The Structurementioning

confidence: 85%

X-ray Rietveld structure refinement of Ca, Sr and Ba meta-antimonates

DeBoer¹,

Young²,

Sakthivel³

1994

Acta Crystallogr C Cryst Struct Commun

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476A12(HPO3)3 AND Ga2(HPO3)3The H-atom positional and displacement parameters were left unrefined. Final observed, calculated and difference profile plots are shown in Fig. 2.MPA would like to acknowledge the University of California for the provision of a scholarship. REM would like to thank the SERC and Blackwell's of Oxford for financial assistance. Some of the work reported here was performed at the Chemical Crystallography Laboratory, University of Oxford, England.

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Section: The Structurementioning

confidence: 85%

X-ray Rietveld structure refinement of Ca, Sr and Ba meta-antimonates

DeBoer¹,

Young²,

Sakthivel³

1994

Acta Crystallogr C Cryst Struct Commun

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“…Metavanadate MeV 2 O 6 (Me = divalent metal ions) compounds at normal pressures have the brannerite structure and a rich variety of possible polymorphs that are dependent on pressure and temperature, that is, orthorhombic columbite ( Pbcn ), tetragonal trirutile ( P 4 2 / mmm ), and trigonal PbSb 2 O 6 ( P 3̅1 m ) structures have been reported . Beck developed the coordination number rule and the rule of hardness to rationalize inorganic coordination structures and the available structures for the compounds with AB 2 O 6 stoichiometry, as occurs in ZnV 2 O 6 , and this author proposes the following polymorphs: CaAs 2 O 6 ( P 321), FeNb 2 O 6 ( Pbcn ), CaV 2 O 6 ( C 2/ m ), SrV 2 O 6 ( Pnma ), BaV 2 O 6 ( C 222), HgV 2 O 6 ( Pbca ) NiV 2 O 6 , ( P 1̅), MoLa 2 O 6 ( I 4̅2 m ), ThTi 2 O 6 ( C 2/ c ), and ThTi 2 O 6 ( C 2/ m ) …”

Section: Introductionmentioning

confidence: 99%

“…28 Metavanadate MeV 2 O 6 (Me = divalent metal ions) compounds at normal pressures have the brannerite structure and a rich variety of possible polymorphs that are dependent on pressure and temperature, that is, orthorhombic columbite (Pbcn), 29 tetragonal trirutile (P4 2 /mmm), and trigonal PbSb 2 O 6 (P3̅ 1m) structures have been reported. 30 Beck 31 developed the coordination number rule and the rule of hardness to rationalize inorganic coordination structures and the available structures for the compounds with AB 2 O 6 stoichiometry, as occurs in ZnV 2 O 6 , and this author proposes the following polymorphs: CaAs 2 O 6 (P321), 32 FeNb 2 O 6 (Pbcn), 33 CaV 2 O 6 (C2/m), 34 SrV 2 O 6 (Pnma), 35 BaV 2 O 6 (C222), 36 HgV 2 O 6 (Pbca) 37 NiV 2 O 6 , (P1̅ ), 38 MoLa 2 O 6 (I4̅ 2m), 39 ThTi 2 O 6 (C2/c), 40 and ThTi 2 O 6 (C2/m). 41 ZnV 2 O 6 is a representative member of the AB 2 O 6 family 30 and has been studied intensively because of its technological importance, and very recently Butt et al 42 and Sun et al 43 reported large-scale synthesis of ZnV 2 O 6 nanostructures, highlighting its potential as a material for energy storage/ conversion.…”

Section: Introductionmentioning

confidence: 99%

Polymorphs of ZnV₂O₆ under Pressure: A First-Principle Investigation

2019

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This work presents first-principle calculations on the pressure-dependence of the stabilities, structures, and electronic properties of several polymorphs of ZnV2O6 under the pressure range 0-30 GPa. These properties are analyzed and discussed in detail using the different parameterizations of the exchange-correlation functional (B3LYP, HSE06, and PBE), and the results are compared with available experimental data. An extensive search process was carried out on the potential energy surface for a set of twelve possible polymorphs. Ten of them are stationary points, but only five have positive frequency values in the range of 0-30 GPa, i.e., monoclinic brannerite (C2/m and C2), orthorhombic columbite (Pbcn), trigonal CaAs2O6-type (P321), and triclinic NiV2O6-type (P1 ̅). The monoclinic ThTi2O6-type (C2/c) phase presents a very low imaginary frequency around 50 cm-1. Orthorhombic SrV2O6-type and BaV2O6-type, tetragonal trirutile and trigonal PbSb2O6-type structures show several imaginary negative frequencies between-400 and-100 cm-1. These imaginary frequencies are indicative of structural instabilities. All attempts to try to converge the calculations to obtain the MoLa2O6-type and HgV2O6-type polymorphs, by using the three functionals, have been unsuccessful. For both brannerite,ThTi2O6-type, columbite, CaAs2O6-type, NiV2O6-type structures numerical and analytical fittings were performed to obtain the lattice parameters, the bulk modulus, B, and their pressure derivative, B′, and the energy-volume relationship of phases are analyzed. Vibrational calculations were performed at each pressure for each polymorph and compared with available experimental data. This study reports, for the first time, a complex and unexpected structural and chemical behavior as a function of pressure. An analysis of the results shows that brannerite monoclinic polymorphs present similar energies, suggesting that both structures may coexist in the range of pressures that were studied. Theoretical prediction reveals that, as the pressure increases, the most stable polymorph of ZnV2O6 moves from the monoclinic phase, C2/m (and C2), to the orthorhombic columbite structure (Pbcn) and the corresponding transition pressure is computed to be 5 GPa at the B3LYP level; however, using the HSE06 and PBE functionals, the FeNb2O6-type structure is the most stable polymorph from ambient pressure up to 30 GPa. In addition the calculations show that the ThTi2O6-type phase (C2/c) becomes more stable than the other two monoclinic structures above 15, 13, and 8 GPa using the B3LYP, HSE06, and PBE functionals, respectively. The findings reported here indicate that the method used to predict relative phase stabilities and phase transitions should be chosen carefully, and that the results should be scrutinized with a critical eye. We analyze the variations of different vibrational frequencies and V−O and Zn−O bond lengths as pressure is applied, and the results confirm that Badger's lineal relationships were not found for the monoclinic polymorphs (C2/m, C2, an...

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“…In an e!ort to resolve this discrepancy, two fairly recent structure determinations have been conducted. The "rst study involved determination of the CaAs O structure from powder X-ray di!raction data (12). In that study, re"nements using P3 1m resulted in unrealistic oxygen positions, leading to the conclusion that P312 was indeed the correct space group (10).…”

Section: Introductionmentioning

confidence: 99%