1992
DOI: 10.1524/zkri.1992.200.1-2.47
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Structural phase transition in GaMo4Se8and AlMo4S8by X-ray powder diffraction

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Cited by 12 publications
(7 citation statements)
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“…Consequently, the orbital degeneracy is lifted by a symmetry lowering cooperative Jahn-Teller distortion in the temperature range between 30 and 50 K, depending on the compounds. This results in rhombohedral R3m (GaV 4 S 8 , GaMo 4 S 8 , GaV 4 Se 8 , GaMo 4 Se 8 , AlMo 4 S 8 ) [4,[9][10][11][12], tetragonal P 42 1 m (GaNb 4 S 8 , GaTa 4 Se 8 ) [13,14], or orthorhombic Imm2 (GeV 4 S 8 ) [9,15] low temperature symmetries.…”
Section: Introductionmentioning
confidence: 99%
“…Consequently, the orbital degeneracy is lifted by a symmetry lowering cooperative Jahn-Teller distortion in the temperature range between 30 and 50 K, depending on the compounds. This results in rhombohedral R3m (GaV 4 S 8 , GaMo 4 S 8 , GaV 4 Se 8 , GaMo 4 Se 8 , AlMo 4 S 8 ) [4,[9][10][11][12], tetragonal P 42 1 m (GaNb 4 S 8 , GaTa 4 Se 8 ) [13,14], or orthorhombic Imm2 (GeV 4 S 8 ) [9,15] low temperature symmetries.…”
Section: Introductionmentioning
confidence: 99%
“…AlV 4 S 8 40 [26] 10 [26] R3m [26] GaV 4 S 8 44 [33] 13 [33] R3m [20] GaV 4 Se 8 41 [31] 18 [31] R3m [26] AlMo 4 S 8 45 [92] 12 [92] R3m [92] GaNb 4 S 8 31 [24] P2 1 2 1 2 1 [13] GaNb 4 Se 8 50* [36] 33 [36] P2 1 2 1 2 1 [37] GaMo 4 S 8 45 [20] 20 [20] R3m [20] GaMo 4 Se 8 54 [93] 25 [93] R3m [92] GaTa 4 Se 8 53 [36] P2 1 2 1 2 1 [37] GeV 4 S 8 30 [76] 15 [76] Imm2 [39] We want to point out that the first lacunar spinel which was shown to become ferroelectric upon the structural transition was GeV 4 S 8 [8] . However, in contrast to all aforementioned lacunar spinels, the highest molecular orbital level of the M 4 cluster in this compound is occupied by two unpaired electrons with total spin S ¼ 1.…”
Section: Introductionmentioning
confidence: 99%
“…A class of model uniaxial skyrmion hosts that exemplifies the rich topology of skyrmionic phase diagrams is the lacunar spinel family of structures. These compounds are defined by tetrahedral clusters of transition metals with a collective spin state that undergo a distortion from F43m to R3m or Imm2 symmetry upon cooling [21][22][23]. This structural symmetry breaking leads to the emergence of magnetic Dzyaloshinskii-Moriya interactions.…”
Section: Introductionmentioning
confidence: 99%