Research/Sitter/MAGNDATA / 0.405_CsCoF4.mcif
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| Magnetic group | I 4′ BNS 82.41 |
| Parent space group | I 4 c 2 No. 120 |
| Spins | collinear · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 12.4353 · b 12.4353 · c 12.8612 Å · α 90° · β 90° · γ 90° |
| Transition | 54 K (−219 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Co |
| Largest moment component | 3.5 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Cs1 | Cs | 0 | 0 | 0.25 | ||||
| Cs2_1 | Cs | 0.3433 | 0.8341 | 0.6799 | ||||
| Cs2_2 | Cs | 0.3433 | 0.1659 | 0.1799 | ||||
| Co1 | Co | 0.5 | 0 | 0 | 0 | 0 | 3.5 | 3.5 |
| Co2_1 | Co | 0.7932 | 0.0749 | 0.9861 | 0 | 0 | −2.8 | 2.8 |
| Co2_2 | Co | 0.7932 | 0.9251 | 0.4861 | 0 | 0 | 3.5 | 3.5 |
| F1_1 | F | 0.3432 | 0.0014 | 0.9899 | ||||
| F1_2 | F | 0.3432 | 0.9986 | 0.4899 | ||||
| F2_1 | F | 0.1412 | 0.0655 | 0.9912 | ||||
| F2_2 | F | 0.1412 | 0.9345 | 0.4912 | ||||
| F3_1 | F | 0.0767 | 0.2094 | 0.1444 | ||||
| F3_2 | F | 0.0767 | 0.7906 | 0.6444 | ||||
| F4_1 | F | 0.9197 | 0.7912 | 0.8632 | ||||
| F4_2 | F | 0.9197 | 0.2088 | 0.3632 | ||||
| F5 | F | 0.7208 | 0.2208 | 0 | ||||
| F6_1 | F | 0 | 0.5 | 0.1433 | ||||
| F6_2 | F | 0 | 0.5 | 0.6433 |
Moment components are along the crystal axes a, b, c (μB), as magCIF writes them. Symmetry generates the rest of the cell from these sites.
P. Lacorre et al. JOURNAL OF SOLID STATE CHEMISTRY (1991) · doi:10.1016/0022-4596(91)90271-I
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.405_CsCoF4.mcif from MAGNDATA · entry page
sha256 of this copy: 44b94287e38633141e71950074f710d18b167799f93dcba231ce44e33eb3149b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.405_CsCoF4.mcif.