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Title: Superspace-group approach to the phase transition of Cu[sub 8]GeSe[sub 6]

Journal Article · · Journal of Solid State Chemistry
; ; ;  [1]; ;  [2]
  1. National Inst. for Research in Inorganic Materials, Namiki, Tsukuba (Japan)
  2. Univ. of Lausanne (Switzerland). Inst. of Crystallography

The high- and low-temperature forms, i.e., phase I (stable above 328 K) and phase II (stable below 328 K), of Cu[sub 8]GeSe[sub 6] have been investigated by the powder X-ray diffraction method. Cu[sub 8]GeSe[sub 6] II is hexagonal with A = 12.6438(2), C = 11.7570(1) [angstrom], Z = 6, and P6[sub 3]cm, and its structure is considered to be a superstructure of the high-temperature form, Cu[sub 8]GeSe[sub 6] I (hexagonal, a = 7.3164(4) [approx equal] A/[radical]3, c = 11.7679(7) [angstrom], Z = 2, and P6[sub 3]mc). Rietveld analysis of Cu[sub 8]GeSe[sub 6] I (350 K) and II (290 K) has been performed using diffraction data measured by a high-resolution powder diffractometer and synchrotron X-ray radiation. For Cu[sub 8]GeSe[sub 6] II, a four-dimensional superspace group for commensurate modulation, P6[sub 3]mc (1/3 1/3 0), with basic cell constants a = 7.2999, c = 11.7570 [angstrom] has been successfully applied (R[sub wp] = 0.054). The superspace-group description allows uniform treatment of both forms, and the phase transition of Cu[sub 8]GeSe[sub 6] is explained in terms of the presence and absence of commensurate modulation waves.

OSTI ID:
6103655
Journal Information:
Journal of Solid State Chemistry, Vol. 146:2; ISSN 0022-4596
Country of Publication:
United States
Language:
English