Research/Sitter/MAGNDATA / 0.1178_Cu2Cl(OH)3.mcif
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| Magnetic group | P c BNS 7.24 |
| Point group | m1 |
| Parent space group | P 21/n No. 14 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 6.1675 · b 6.8327 · c 9.1517 Å · α 90° · β 99.492° · γ 90° |
| Transition | 18.1 K (−255 °C) |
| Measured at | 1.7 K |
| Magnetic ions | Cu |
| Largest moment component | 0.3 μB |
| Method | SND |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Cu1 | Cu | 0 | 0.5 | 0.5 | −0.3 | 0 | −0.29 | 0.3813 |
| Cu2 | Cu | 0 | 0 | 0 | 0.3 | 0 | 0.29 | 0.3813 |
| Cu3_1 | Cu | 0.2648 | 0.2373 | 0.7521 | 0.29 | 0.25 | 0 | 0.3829 |
| Cu3_2 | Cu | 0.2352 | 0.7373 | 0.7479 | 0.29 | −0.25 | 0 | 0.3829 |
| Cl1_1 | Cl | 0.1118 | 0.9925 | 0.303 | ||||
| Cl1_2 | Cl | 0.3882 | 0.4925 | 0.197 | ||||
| O1_1 | O | 0.2975 | 0.2963 | 0.5483 | ||||
| O1_2 | O | 0.2025 | 0.7963 | 0.9517 | ||||
| O2_1 | O | 0.4168 | 0.9703 | 0.771 | ||||
| O2_2 | O | 0.0832 | 0.4703 | 0.729 | ||||
| O3_1 | O | 0.2484 | 0.6811 | 0.5378 | ||||
| O3−2 | O | 0.2516 | 0.1811 | 0.9622 | ||||
| H1_1 | H | 0.2881 | 0.1807 | 0.4888 | ||||
| H1_2 | H | 0.2119 | 0.6807 | 0.0112 | ||||
| H2_1 | H | 0.5383 | 0.9555 | 0.7181 | ||||
| H2_2 | H | 0.9617 | 0.4555 | 0.7819 | ||||
| H3_1 | H | 0.2286 | 0.7885 | 0.4698 | ||||
| H3_2 | H | 0.2714 | 0.2885 | 0.0302 |
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.
L. Stodter et al. Phys. Rev. Lett. (2026) · doi:10.1103/xmh8-68vk
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.1178_Cu2Cl(OH)3.mcif from MAGNDATA · entry page
sha256 of this copy: 6270522d98f28656ddd92f26c9993904fa6ac6180feed61ebc2711ee965d853e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1178_Cu2Cl(OH)3.mcif.