Research/Sitter/MAGNDATA / 1.1.77_NiBr2.mcif
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| Magnetic group | Rm1′(ααγ)0s |
| Point group | m1′ |
| Parent space group | R 3m No. 166 |
| Repeats every | 0.67 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0.027 0.027 1.5] 1k |
| Cell | a 3.723 · b 3.723 · c 18.34 Å · α 90° · β 90° · γ 120° |
| Transition | 22.8 K (−250 °C) |
| Measured at | 4.2 K |
| Magnetic ions | Ni |
| Largest moment component | 2 μB |
| Method | NSD and NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ni1 | Ni | 0 | 0 | 0 | ||||
| Br1_1 | Br | 0 | 0 | 0.255 | ||||
| Br1_2 | Br | 0 | 0 | −0.255 |
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.
A. Adam et al. Solid State Communications (1980) · doi:10.1016/0038-1098(80)90757-7
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.77_NiBr2.mcif from MAGNDATA · entry page
sha256 of this copy: d8d0798c6f5753f9bb34f0d6bfc5b32c1d4b8f9a44da5029ebb241d6695539a2
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.77_NiBr2.mcif.