Research/Sitter/MAGNDATA / 1.1.144_CePdAl.mcif
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| Magnetic group | Xm2m1′(0,0,γ)000s |
| Point group | mm21′ |
| Parent space group | P 6 2 m No. 189 |
| Repeats every | 2.86 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.35] 1k |
| Cell | a 12.46211 · b 7.195 · c 4.24 Å · α 90° · β 90° · γ 90° |
| Transition | 2.7 K (−270 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Ce |
| Largest moment component | 1.58 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ce1_1 | Ce | 0.2893 | 0.7107 | 0 | ||||
| Ce1_2 | Ce | 0 | 0.5785 | 0 | ||||
| Pd1_1 | Pd | 0 | 0 | 0 | ||||
| Pd2_1 | Pd | 0.1667 | 0.5 | 0.5 | ||||
| Al1_1 | Al | 0.114 | 0.886 | 0.5 | ||||
| Al1_2 | Al | 0 | 0.228 | 0.5 |
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.
A. Donni et al. J. Phys.: Condens. Matter (1996) · doi:10.1088/0953-8984/8/50/043
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.144_CePdAl.mcif from MAGNDATA · entry page
sha256 of this copy: cf08b95eb224107d845c3f349dc27f23adb3c5c6ed9a42dbfff6e15b55efa890
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.144_CePdAl.mcif.