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Investigation of (Sr4−δCaδ)PtO6 using X-ray Rietveld refinement

Published online by Cambridge University Press:  10 January 2013

W. Wong-Ng
Affiliation:
Ceramics Division, National Institute of Standards and Technology, Gaithersburg, Maryland 20899
J. A. Kaduk
Affiliation:
Amoco Corporation, Naperville, Illinois
R. A. Young
Affiliation:
School of Physics, Georgia Institute of Technology, Atlanta, Georgia
F. Jiang
Affiliation:
Geology Department, University of Maryland, College Park, Maryland
L. J. Swartzendruber
Affiliation:
Metallurgy Division, National Institute of Standards and Technology, Gaithersburg, Maryland 20899
H. J. Brown
Affiliation:
Metallurgy Division, National Institute of Standards and Technology, Gaithersburg, Maryland 20899

Abstract

The structures of the solid solution series (Sr4−δCaδ)PtO6, with δ=0, 0.85(1), 2, and 3, have been investigated using the Rietveld refinement technique with laboratory X-ray powder diffraction data. A complete solid solution between Sr and Ca was confirmed to exist. These compounds crystallize in the rhombohedral space group Rc. The cell parameters of the series range from a of 9.4780(3) to 9.7477(1) Å, and c from 11.3301(4) to 11.8791(1) Å for δ from 3 to 0, respectively. The structure consists of chains of alternating trigonal prismatic (Sr, Ca)O6 and octahedral PtO6 units running parallel to the c axis. These chains are connected to each other via a second type of (Sr, Ca) ions, which are surrounded by eight oxygens, in a distorted square antiprismatic geometry. As Ca replaced Sr in Sr4PtO6, it was found to substitute preferentially in the smaller octahedral (Sr, Ca)1 site (6a) rather than at the eight-coordinate (Sr, Ca)2 site (18e). There appears to be an anomaly of cell parameters a and c at the compound Sr3.15Ca0.85PtO6. Their dependence on Ca content changes at δ≈1.00, where the Ca has fully replaced Sr in the 6a site. The substitution of Sr by Ca reduced the average (Sr, Ca)1–O length from 2.411 to 2.311 Å and (Sr, Ca)2–O from 2.659 to 2.570 Å as the composition varied from Sr4PtO6 to SrCa3PtO6. Reference X-ray powder diffraction patterns were prepared from the Rietveld refinement results for these members of the solid solution series. Magnetic susceptibility measurements of three of the samples (δ=0, 0.85, 2) show electronic transitions at low temperatures.

Type
Research Article
Copyright
Copyright © Cambridge University Press 1999

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References

Bednorz, J. G., and Muller, K. A. (1986). “Possible High T c Superconductivity in the Ba–La–Cu–O system,” Z. Phys. B 64, 189193.CrossRefGoogle Scholar
Bergerhoff, G., and Schmitz-Dumont, O. (1956). “Die Kristallstruktur des kaliumhexachlorocadnates. II,” Z. Anorg. Allg. Chem. 284, 10.CrossRefGoogle Scholar
Brese, N. E., and O’Keeffe, M. (1991). “Bond Valence Parameters for Solids,” Acta Crystallogr., Sect. B: Struct. Sci. B47, 192.CrossRefGoogle Scholar
Brown, I. D., and Altermatt, D. (1985). “Bond Valence Parameters Obtained from a Systematic Analysis of the Inorganic Crystal Structure Database,” Acta Crystallogr., Sect. B: Struct. Sci. B41, 244247.CrossRefGoogle Scholar
Bykov, A. B., Radaev, S. F., Genkina, E. A., Dem’yanets, L. N., Maximov, B. A., and Mel’nikov, O. K. (1990). “Synthesis and Atomic Structure of the Compound Ca 1.75Sr 1.5Cu 0.75PtO 6, Crystallizing in the Bi–Sr–Ca–Cu–O System of High-Temperature Superconductors,” Kristallografiya 35, 869873ICSD collection code 39282.Google Scholar
Dollase, W. A. (1986). “Correction of intensities for preferred orientation in powder diffractometry: Application of the March model,” J. Appl. Crystallogr. 19, 267272.CrossRefGoogle Scholar
Kaduk, J. A., and Wong-Ng, W. (1996). “Standard X-ray Diffraction Patterns of Technologically-important Materials,” ICDD Grant-in-Aid report.Google Scholar
McDaniel, C. L. (1972). “Phase Relations in the CaO–Pt System in Air,” J. Am. Ceram. Soc. 55, 426.CrossRefGoogle Scholar
Nguyen, T. N., Giaquinta, D. M., and Loyle, H.-C. (1994). “Synthesis of the New One-dimensional Compound Sr 3NiPtO 6: Structure and Magnetic Properties,” Chem. Mater. 6, 16421646.CrossRefGoogle Scholar
Nún˜ez, P., Trail, S., and Loye, H-C. (1997). “Synthesis, Crystal Structure, and Magnetic Properties of Sr 3MgMO 6 (M=Pt, Ir, Rh),” J. Solid State Chem. 130, 3541.CrossRefGoogle Scholar
PDF—Powder Diffraction File (PDF), McClune, W. F., editor, International Centre for Diffraction Data, 12 Campus Blvd., Newtown Square, PA 19073-3273.Google Scholar
Randall, J. J. Jr., and Katz, L. (1959). “The Crystal Structure of Sr 4PtO 6 and Two Related Compounds,” Acta Crystallogr. 12, 519.CrossRefGoogle Scholar
Reardon, B. J., and Hubbard, C. R. (1992a). “A Review of the XRD data of the Phases Present in the CaO–SrO–PbO system,” Powder Diffr. 7, 9698.CrossRefGoogle Scholar
Reardon, B. J., and Hubbard, C. R. (1992b). “A Review of the XRD Data of the Phases present in the CaO–SrO–CuO System,” Powder Diffr. 7, 142.CrossRefGoogle Scholar
Swanson, H. E., McMurdie, H. F., Morris, M. C., Evans, E. H., and Paretzkin, B. (1972). “Standard X-ray Diffraction Powder Patterns,” NBS Monogr. 25, 18.Google Scholar
Schwartz, K. B., Parise, J. B., Prewitt, C. T., and Shannon, R. D. (1982). “Analysis of Structural Distortion in Non-Stoichiometric Ternary Platinum Oxides: Li 0.64Pt 3O 4 and Co 0.37Na 0.14Pt 3O 4,Acta Crystallogr., Sect. B: Struct. Crystallogr. Cryst. Chem. B38, 21092116.CrossRefGoogle Scholar
Schwartz, K. B., Parise, J. B., Prewitt, C. T., and Shannon, R. D. (1983). “Structure and Crystal Chemistry of Mixed-Valence Ternary Platinum Oxides: MnPt 3O 6, CoPt 3O 6, MgPt 3O 6, NiPt 3O 6,Acta Crystallogr., Sect. B: Struct. Sci. B39, 217226.CrossRefGoogle Scholar
Schwartz, K. B., and Prewitt, C. T. (1984). “Structural and Electronic Properties of Binary and Ternary Platinum Oxides,” J. Phys. Chem. Solids 45, 121.CrossRefGoogle Scholar
Segal, N., Vente, J. P., Bush, T. S., and Battle, P. D. (1996). “Structural and magnetic properties of Sr 4−xM xIrO 6 (M=Ca, Zn, Cd, Li, Na),” J. Mater. Chem. 6, 395401.CrossRefGoogle Scholar
von Czaya, R. (1970). “Darstellung und kristallographische Daten von Tetracalciumplatinoxid Ca 4PtO 6,Z. Anorg. Allg. Chem. 375, 62.Google Scholar
Wilkinson, A. P., and Cheetham, A. K. (1989). “The Structure of Ba 4PtO 6 from Time-of-Flight Powder Neutron Diffraction Data,” Acta Crystallogr., Sect. C: Cryst. Struct. Commun. C45, 16721674.CrossRefGoogle Scholar
Wong-Ng, W., Snyder, R. L., Park, C., Antipov, E., and McClune, W. F. (1997). “The ICDD/PDF Superconductor MiniFile (SC),” Powder Diffr. 12, 13.CrossRefGoogle Scholar
Wong-Ng, W. (1992). “The ICDD/PDF Coverage of the High T c Superconductor and Related Compounds in the A–R–Cu–O Systems (A=Ba, Sr and Ca, and R=lanthanides and Y),” Powder Diffr. 7, 125.CrossRefGoogle Scholar
Young, R. A., Sakthivel, A., Moss, T. S., and Paiva Santos, C. O. (1995). “DBWS-9411; an upgrade of the DBWS*.* programs for Rietveld refinement with PC and mainframe computers,” J. Appl. Crystallogr. 28, 366–7.CrossRefGoogle Scholar