Research/Sitter/MAGNDATA / 1.1.115_UPd2Ge2.mcif
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| Magnetic group | I4/mmm1′(0,0,γ)00sss |
| Point group | 4/mmm1′ |
| Parent space group | I 4/m m m No. 139 |
| Repeats every | 1.37 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.7302] 1k |
| Cell | a 4.2 · b 4.2 · c 10.23 Å · α 90° · β 90° · γ 90° |
| Transition | 135 K (−138 °C) |
| Measured at | 100 K |
| Magnetic ions | U |
| Largest moment component | 2.49 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Pd1 | Pd | 0 | 0.5 | 0.25 | ||||
| U1 | U | 0 | 0 | 0 | ||||
| Ge1 | Ge | 0 | 0 | 0.383 |
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. Andre et al. Solid State Communications (1996) · doi:10.1016/0038-1098(95)00818-7
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.115_UPd2Ge2.mcif from MAGNDATA · entry page
sha256 of this copy: 10f24e8da4e16de40b46bf793f5c673ad1f7f97a1120ee6b739189c97ff4da80
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.115_UPd2Ge2.mcif.