The Phase Co1-xNixSn2: Structural Variations Based on the Stacking of Two Different Planar Nets

Inorganic Chemistry

Volumn 36, Issue 20, 1997, Pages 4307-4315

  Häussermann, Ulrich ^a   Landa Cánovas, Angel R ^a,b   Lidin, Sven ^a  

^a LUND UNIVERSITY   (Sweden)

^b UNIVERSIDAD COMPLUTENSE DE MADRID   (Spain)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 0642337654     PISSN: 00201669     EISSN: None     Source Type: Journal    
DOI: 10.1021/ic9703134     Document Type: Article

References (22)

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2. Ferro, R.; Saccone, A. In The Structure of Solids; Cahn, R. W., Haasen, P., Kramer, E. J., Eds.; VCH: Weinheim 1993; Vol. 1, Chapter 3.
3. Hoistad, L. M.; Lee, S. J. Am. Chem. Soc. 1991, 113, 8216.
4. Larsson A.-K.; Lidin, S. J. Alloys Compd. 1995, 221, 136.
5. Häussermann, U.; Lidin, S. Manuscript in preparation.
6. Hyde, B. G.; Andersson, S. Inorganic Crystal Structures; John Wiley & Sons: New York, 1989.
7. Pearson, W. B. The Crystal Chemistry and Physics of Metals and Alloys; John Wiley & Sons: New York, 1972.
8. Jeitschko, W.; Jaberg, B. Acta Crystallogr., Sect. B: Struct. Sci. 1982, B38, 598.
9. Lang, A.; Jeitschko W. Z. Metallkd. 1996, 87, 759.
10. Werner, P.-E. TREOR Trial-and-error program for indexing of unknown powder patterns; University of Stockholm: Stockholm, Sweden, 1988.
11. Sheldrick, G. M. SHELXL-93 Program for the Refinement of Crystal Structures; University of Göttingen: Göttingen, FRG, 1993.
12. Kilaas, R. 45th Annual Proceedings of the Electron Microscopy Society of America, Baltimore, Maryland, 1987; p 66.
13. Schubert, K.; Pfisterer, H. Z. Metallkd. 1950, 41, 433.
14. Panday, P. K.; Schubert, K. J. Less-Common Met. 1969, 18, 175.
15. Villars, P.; Calvert, L. D. Pearsons Handbook of Crystallographic Data for Intermetallic Compounds, 2nd ed.; ASM International: Materials Park, OH, 1991.
16. 2.
17. 2.
18. El-Boragy, M.; Schubert, K. Z. Metallkd. 1971, 62, 667.
19. Schubert, K.; Lukas, H. L.; Meissner, H.-G.; Bhan, S. Z. Metallkd. 1959, 50, 534.
20. 3 structure as the low-temperature form.
21. Double diffraction consists in the redistribution of diffracted intensity in a diffraction pattern by the scattering of an already diffracted electron along any other allowed diffraction path. Consequently, any electron from the diffuse-streaked 21l row, for example, can diffract a second time with the crystal along the 2̄1̄0 diffraction path to add intensity to the 00l reflection row in the final pattern.
22. 2 structure forbids the 36l: l = 2n + 1 and the 63l: l = 2n reflections because of the general condition hkl: k + l = 2n + 1. Reflections forbidden by centering cannot appear by double diffraction.