Research/Sitter/MAGNDATA / 0.1005_Mn3RhGe.mcif
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| Magnetic group | P 21 3 1 BNS 198.9 |
| Point group | 23 |
| Parent space group | P 21 3 No. 198 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 6.601 · b 6.601 · c 6.601 Å · α 90° · β 90° · γ 90° |
| Transition | 225 K (−48 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Mn |
| Largest moment component | 2.2 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Mn1 | Mn | 0.12 | 0.206 | 0.452 | 1.34 | 2.2 | −1.84 | 3.1656 |
| Rh1 | Rh | 0.6862 | 0.6862 | 0.6862 | ||||
| Ge1 | Ge | 0.064 | 0.064 | 0.064 |
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. E. Hall et al. PHYSICAL REVIEW MATERIALS (2023) · doi:10.1103/PhysRevMaterials.7.114402
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.1005_Mn3RhGe.mcif from MAGNDATA · entry page
sha256 of this copy: 1d59ee56a2ee70ad7e551904dc58e3c04dec4c89f3c00e1c534df55645e91ac5
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1005_Mn3RhGe.mcif.