Research/Sitter/MAGNDATA / 1.1.116_UPd2Si2.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 0.732] 1k |
| Cell | a 4.2 · b 4.2 · c 10.23 Å · α 90° · β 90° · γ 90° |
| Transition | 136 K (−137 °C) |
| Measured at | 120 K |
| Magnetic ions | U |
| Largest moment component | 2.3 μB |
| Method | NSPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Pd1 | Pd | 0 | 0.5 | 0.25 | ||||
| U1 | U | 0 | 0 | 0 | ||||
| Si1 | Si | 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.
B. Shemirani et al. PHYSICAL REVIEW B (1993) · doi:10.1103/PhysRevB.47.8672
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.116_UPd2Si2.mcif from MAGNDATA · entry page
sha256 of this copy: 4a00fb8abf619c69b2f26da6868b7bf5975c00cf046b1a57a9263977d07bf1fb
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.116_UPd2Si2.mcif.