Research/Sitter/MAGNDATA / 1.51_Cs2CoCl4.mcif
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| Magnetic group | Pa 21 BNS 4.10 |
| Point group | 21′ |
| Parent space group | P n m a No. 62 |
| Spins | coplanar · net moment 0 μB per cell |
| Propagation | [0 1/2 1/2] 1k |
| Cell | a 9.72 · b 14.626 · c 25.644 Å · α 90° · β 90° · γ 90° |
| Transition | 0.217 K (−273 °C) |
| Measured at | 0.08 K |
| Magnetic ions | Co |
| Largest moment component | 1.6 μB |
| Method | NSD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Cs1_1 | Cs | 0.3599 | 0.125 | 0.0504 | ||||
| Cs1_2 | Cs | 0.6401 | −0.125 | −0.0504 | ||||
| Cs2_1 | Cs | 0.0222 | 0.125 | −0.0882 | ||||
| Cs2_2 | Cs | −0.0222 | −0.125 | 0.0882 | ||||
| Co1_1 | Co | 0.7649 | 0.125 | 0.0389 | 0 | −1.6 | −0.4 | 1.6492 |
| Co1_2 | Co | 0.2351 | −0.125 | −0.0389 | 0 | −1.6 | 0.4 | 1.6492 |
| Cl1_1 | Cl | −0.0037 | 0.125 | 0.05 | ||||
| Cl1_2 | Cl | 0.0037 | 0.375 | 0.45 | ||||
| Cl2_1 | Cl | 0.6877 | 0.125 | 0.4556 | ||||
| Cl2_2 | Cl | 0.3123 | 0.375 | 0.0444 | ||||
| Cl31_1 | Cl | 0.674 | 0.2509 | 0.0764 | ||||
| Cl31_2 | Cl | 0.326 | −0.2509 | −0.0764 | ||||
| Cl32_1 | Cl | 0.826 | 0.2491 | 0.3264 | ||||
| Cl32_2 | Cl | 0.174 | 0.2509 | 0.1736 |
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.
M. Kenzelmann et al. PHYSICAL REVIEW B (2002) · doi:10.1103/physrevb.65.144432
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.51_Cs2CoCl4.mcif from MAGNDATA · entry page
sha256 of this copy: ca7b51be9d2f8046782c8d04e73b58c0aa1175ae24f0fa31b5040b9263b91664
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.51_Cs2CoCl4.mcif.