Research/Sitter/MAGNDATA / 1.1.120_Er3Cu4Sn4.mcif
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| Magnetic group | C2/m1′c(0,β,0)s00 |
| Point group | 2/m1′ |
| Parent space group | C 2/m No. 12 |
| Repeats every | 1.88 cells along b (not a whole number: that's what incommensurate means) |
| Propagation | [0 0.5333 0] 2k |
| Cell | a 16.0831 · b 4.3887 · c 13.7464 Å · α 90° · β 115.754° · γ 90° |
| Transition | 2 K (−271 °C) |
| Measured at | 1.4 K |
| Magnetic ions | Er |
| Largest moment component | 9.6 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Er1 | Er | 0 | 0 | 0.25 | 0 | 8.91 | 0 | 8.91 |
| Er2 | Er | 0.13 | 0 | 0.0595 | ||||
| Cu1 | Cu | 0.322 | 0 | 0.2575 | ||||
| Cu2 | Cu | 0.338 | 0 | 0.078 | ||||
| Sn1 | Sn | 0.216 | 0 | 0.364 | ||||
| Sn2 | Sn | 0.507 | 0 | 0.1055 |
Incommensurate: the moments are modulated; the picture evaluates each atom's Fourier series at its own phase.
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.
S. Baran et al. Acta Cryst. B (2021) · doi:10.1107/S205252062100127X
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.120_Er3Cu4Sn4.mcif from MAGNDATA · entry page
sha256 of this copy: 0d652154e6a624fc6374ffc320a064a2440f7f347cda56bbc9825fe12bbc9ea3
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.120_Er3Cu4Sn4.mcif.