Research/Sitter/MAGNDATA / 1.1.10_DyMn6Ge6.mcif
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| Magnetic group | P62′2′(00γ)h00 |
| Point group | 62′2′ |
| Parent space group | P 6/m m m No. 191 |
| Repeats every | 6.06 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.1651] 1k |
| Cell | a 5.2081 · b 5.2081 · c 8.1522 Å · α 90° · β 90° · γ 120° |
| Magnetic ions | Dy, Mn |
| Largest moment component | 7.154 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Dy1 | Dy | 0 | 0 | 0 | 0 | 0 | 3.932 | 3.932 |
| Mn1 | Mn | 0.5 | 0 | 0.251 | 0 | 0 | −1.149 | 1.149 |
| Ge1 | Ge | 0.3333 | 0.6667 | 0 | ||||
| Ge2 | Ge | 0.3333 | 0.6667 | 0.5 | ||||
| Ge3 | Ge | 0 | 0 | 0.3447 |
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.
J. Rodriguez-Carvajal et al. EPJ Web of Conferences (2012) · doi:10.1051/epjconf/20122200010
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.10_DyMn6Ge6.mcif from MAGNDATA · entry page
sha256 of this copy: c4077673d8daa3e60bf37f20504dbb85fcf83b9fda29d697bf2564dde3ca100f
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.10_DyMn6Ge6.mcif.