Research/Sitter/MAGNDATA / 1.739_Cu9O2(SeO3)4Cl6.mcif
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| Magnetic group | PS 1 BNS 2.7 |
| Point group | 11′ |
| Parent space group | C 2/m No. 12 |
| Spins | coplanar · net moment 0 μB per cell |
| Propagation | [1/2 1/2 0] 1k |
| Cell | a 29.8834 · b 12.5298 · c 12.9387 Å · α 90° · β 120.03° · γ 90° |
| Transition | 37 K (−236 °C) |
| Measured at | 4 K |
| Magnetic ions | Cu |
| Largest moment component | 0.55 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Cu1 | Cu | 0 | 0 | 0 | 0.55 | 0 | −0.3 | 0.7468 |
| Cu2 | Cu | 0.0585 | 0 | 0.282 | 0.55 | 0 | −0.3 | 0.7468 |
| Cu3 | Cu | 0.108 | 0 | 0.771 | 0.55 | 0 | −0.3 | 0.7468 |
| Cu4 | Cu | 0.191 | 0 | 0.41 | −0.55 | 0 | −0.3 | 0.4768 |
| Cu5_1 | Cu | 0.125 | 0.125 | 0.5 | ||||
| Cu5_2 | Cu | 0.375 | 0.125 | 0.5 | 0.55 | 0 | −0.3 | 0.7468 |
| Se1 | Se | 0.1255 | 0 | 0.138 | ||||
| Se2 | Se | 0.269 | 0 | 0.302 | ||||
| O1 | O | 0.13 | 0 | 0.421 | ||||
| O2_1 | O | 0.063 | 0.1485 | 0.339 | ||||
| O2_2 | O | 0.937 | 0.1485 | 0.661 | ||||
| O3_1 | O | 0.154 | 0.0965 | 0.236 | ||||
| O3_2 | O | 0.846 | 0.0965 | 0.764 | ||||
| O4 | O | 0.0665 | 0 | 0.133 | ||||
| O5 | O | 0.2565 | 0 | 0.413 | ||||
| Cl1 | Cl | 0.066 | 0 | 0.568 | ||||
| Cl2 | Cl | 0.027 | 0 | 0.86 | ||||
| Cl3 | Cl | 0.32 | 0 | 0.046 |
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.
H. C. Wu et al. PHYSICAL REVIEW B (2019) · doi:10.1103/PhysRevB.100.245119
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.739_Cu9O2(SeO3)4Cl6.mcif from MAGNDATA · entry page
sha256 of this copy: bc0177a6a72b8f589aa35eb83b017917941625c88d05cbe782ecc357fc725abf
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.739_Cu9O2(SeO3)4Cl6.mcif.