Research/Sitter/MAGNDATA / 1.1.55_CeCu2Ge2.mcif
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| Magnetic group | I21′(α,α,γ)0s |
| Point group | 21′ |
| Parent space group | I 4/m m m No. 139 |
| Repeats every | 1.85 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0.28 0.28 0.54] 1k |
| Cell | a 4.158 · b 4.158 · c 10.227 Å · α 90° · β 90° · γ 90° |
| Transition | 4.1 K (−269 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Ce |
| Largest moment component | 0.65 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ce1 | Ce | 0 | 0 | 0 | ||||
| Cu1_1 | Cu | 0 | 0.5 | 0.25 | ||||
| Cu1_2 | Cu | 0 | −0.5 | −0.25 | ||||
| Ge1 | Ge | 0 | 0 | 0.385 |
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.
G. Knopp et al. Z. Phys. B - Condensed Matter (1989) · doi:10.1007/BF01313625
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.55_CeCu2Ge2.mcif from MAGNDATA · entry page
sha256 of this copy: 9eff65c3f4b73aa2cbbd2cb5641eee267c34405b795ce7980921b17b1bd1da1a
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.55_CeCu2Ge2.mcif.