Ni1Cr1O4
MAGNDATA entry 2.93 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Research/Sitter/MAGNDATA / 2.93_CoCrO4.mcif
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| Magnetic group | P b c n BNS 60.417 |
| Point group | mmm |
| Parent space group | C m c m No. 63 |
| Spins | coplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] · [1 0 0] 1k |
| Cell | a 5.524 · b 8.308 · c 6.234 Å · α 90° · β 90° · γ 90° |
| Measured at | 4.2 K |
| Magnetic ions | Co |
| Largest moment component | 0.98 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Co1 | Co | 0 | 0 | 0 | 0.69 | 0 | 0.98 | 1.1985 |
| Cr1 | Cr | 0 | 0.357 | 0.25 | ||||
| O1 | O | 0 | 0.24 | 0.033 | ||||
| O2 | O | 0.25 | 0.472 | 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. Pernet et al. Bull. Soc. fr. Mineral. (1969) · doi:10.3406/bulmi.1969.6355
Cite the original paper and MAGNDATA, not this mirror.
⬇ 2.93_CoCrO4.mcif from MAGNDATA · entry page
sha256 of this copy: de6ab66a17f365866dfafdbfad04313f7b142aa44637564f10072e897a3418ec
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.93_CoCrO4.mcif.