Research/Sitter/MAGNDATA / 1.1.46_ScMn6Ge6.mcif
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| Magnetic group | P6221′c(00γ)h00s |
| Point group | 6221′ |
| Parent space group | P 6/m m m No. 191 |
| Repeats every | 1.23 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.81] 1k |
| Cell | a 5.1684 · b 5.1684 · c 16.794 Å · α 90° · β 90° · γ 120° |
| Transition | 100 K (−173 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Mn |
| Largest moment component | 2.09 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Sc1 | Sc | 0 | 0 | 0 | ||||
| Mn1 | Mn | 0.5 | 0 | 0.1229 | 0 | 0 | 2.09 | 2.09 |
| Ge1 | Ge | 0.3333 | 0.6667 | 0.25 | ||||
| Ge2 | Ge | 0.3333 | 0.6667 | 0 | ||||
| Ge3 | Ge | 0 | 0 | 0.1693 |
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.
P. Schobinger-Papamantellos et al. Journal of Magnetism and Magnetic Materials (2014) · doi:10.1016/j.jmmm.2014.06.052
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.46_ScMn6Ge6.mcif from MAGNDATA · entry page
sha256 of this copy: 75310334b7f68e60ba6fc02466664df0baf20b979eddcfb8c82cf2fc35df1c37
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.46_ScMn6Ge6.mcif.