Research/Sitter/MAGNDATA / 1.1.121_ScFeGe.mcif
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| Magnetic group | P3211′(0,0,γ)-t00s |
| Point group | 321′ |
| Parent space group | P 6 2 m No. 189 |
| Repeats every | 5.18 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.193] 1k |
| Cell | a 6.5429 · b 6.5429 · c 3.8915 Å · α 90° · β 90° · γ 120° |
| Transition | 36 K (−237 °C) |
| Measured at | 4 K |
| Magnetic ions | Fe |
| Largest moment component | 0.612 μB |
| Method | NSD and NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Fe1 | Fe | 0.7698 | 0.7698 | 0 | ||||
| Sc1 | Sc | 0.4196 | 0.4196 | 0.5 | ||||
| Ge1 | Ge | 0 | 0 | 0.5 | ||||
| Ge2 | Ge | 0.6667 | 0.3333 | 0 |
Incommensurate: the moments are modulated; the picture evaluates each atom's Fourier series at its own phase.
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. K. Karna et al. PHYSICAL REVIEW B (2021) · doi:10.1103/PhysRevB.103.014443
Cite the original paper and MAGNDATA, not this mirror.
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sha256 of this copy: 19dd85432641825ff6a53e3da5f862f3a179da725c9ded2b79bfce35a90a22b2
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.121_ScFeGe.mcif.