Research/Sitter/MAGNDATA / 1.2_CuSe2O5.mcif
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| Magnetic group | Pc 21/c BNS 14.84 |
| Point group | 2/m1′ |
| Parent space group | C 2/c No. 15 |
| Spins | coplanar · net moment 0 μB per cell |
| Propagation | [1 0 0] 1k |
| Cell | a 12.254 · b 4.858 · c 7.96 Å · α 90° · β 110.7° · γ 90° |
| Transition | 17 K (−256 °C) |
| Measured at | 6 K |
| Magnetic ions | Cu |
| Largest moment component | 0.5 μB |
| Method | NSD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Cu1 | Cu | 0 | 0 | 0 | 0.13 | 0.5 | 0 | 0.5166 |
| Se1 | Se | 0.1399 | −0.4353 | 0.3299 | ||||
| O1 | O | 0.1258 | 0.2251 | −0.0131 | ||||
| O2 | O | 0.1256 | −0.2237 | 0.1584 | ||||
| O3 | O | 0 | −0.6168 | 0.25 |
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. Herak et al. Phys. Rev. B (2013) · doi:10.1103/physrevb.87.104413
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.2_CuSe2O5.mcif from MAGNDATA · entry page
sha256 of this copy: e153603dcb1d021e4674bd492392429b5bf3710adc172832169169e6b9b21209
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.2_CuSe2O5.mcif.