Rb1Ru1O4
MAGNDATA entry 0.924 · 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 / 0.924_RbRuO4.mcif
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| Magnetic group | P n′ m′ a′ BNS 62.449 |
| Point group | m′m′m′ |
| Parent space group | P n m a No. 62 |
| Spins | coplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 5.5082 · b 5.7502 · c 13.7683 Å · α 90° · β 90° · γ 90° |
| Measured at | 3 K |
| Magnetic ions | Ru |
| Largest moment component | 0.77 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Rb1 | Rb | 0.0264 | 0.25 | 0.125 | ||||
| Ru1 | Ru | 0.9616 | 0.25 | 0.625 | −0.21 | 0 | 0.77 | 0.7981 |
| O1 | O | 0.1639 | 0.25 | 0.918 | ||||
| O2 | O | 0.6428 | 0.25 | 0.9801 | ||||
| O3 | O | 0.9805 | 0.9946 | 0.3128 |
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. Injac et al. Inorg. Chem. (2020) · doi:10.1021/acs.inorgchem.9b03118
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.924_RbRuO4.mcif from MAGNDATA · entry page
sha256 of this copy: 02fa1815210ad6cca174449175a823dcc76d979119667d4dbf0e83319c62e1f6
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.924_RbRuO4.mcif.