Research/Sitter/MAGNDATA / 2.71_HoRh.mcif
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| Magnetic group | PC 21/m BNS 11.57 |
| Parent space group | P m 3 m No. 221 |
| Spins | coplanar · net moment 0 μB per cell |
| Propagation | [0 0 1/2] · [0 1/2 0] · [1/2 0 0] 2k |
| Cell | a 6.754 · b 6.754 · c 3.377 Å · α 90° · β 90° · γ 90° |
| Transition | 3.2 K (−270 °C) |
| Measured at | 1.2 K |
| Magnetic ions | Ho |
| Largest moment component | 3 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ho1 | Ho | 0 | 0 | 0 | 3 | 3 | 3 | 5.1962 |
| Rh1_1 | Rh | 0.25 | 0.25 | 0.5 | ||||
| Rh1_2 | Rh | 0.25 | 0.75 | 0.5 |
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.
R. Chamard-Bois et al. Solid State Communications (1972) · doi:10.1016/0038-1098(72)90586-8
Cite the original paper and MAGNDATA, not this mirror.
⬇ 2.71_HoRh.mcif from MAGNDATA · entry page
sha256 of this copy: 9ef2ef43622b2eeea67bd6b6c30712de55fb5585af01d6b577216b52c5c13406
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.71_HoRh.mcif.