Research/Sitter/MAGNDATA / 0.900_Mn3CoGe.mcif
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| Magnetic group | P 21 3 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 6.3742 · b 6.3742 · c 6.3742 Å · α 90° · β 90° · γ 90° |
| Transition | 145 K (−128 °C) |
| Measured at | 10 K |
| Magnetic ions | Co, Mn |
| Largest moment component | 1.52 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Mn1 | Mn | 0.1254 | 0.2022 | 0.4532 | 1.03 | 1.52 | −1.52 | 2.3836 |
| Co1 | Co | 0.6848 | 0.6848 | 0.6848 | ||||
| Ge1 | Ge | 0.0642 | 0.0642 | 0.0642 |
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.
T. Eriksson et al. PHYSICAL REVIEW B (2005) · doi:10.1103/PhysRevB.72.144427
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.900_Mn3CoGe.mcif from MAGNDATA · entry page
sha256 of this copy: 6923f45d91bff37763ee3fcad17f671c816a82c67894231f0928b9ba658c7e95
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.900_Mn3CoGe.mcif.