Research/Sitter/MAGNDATA / 1.1.143_CeRh0.25Pd0.75Sn.mcif
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| Magnetic group | P62m1′(0,0,γ)00ss |
| Point group | 6m21′ |
| Parent space group | P 6 2 m No. 189 |
| Repeats every | 2.56 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.39] 1k |
| Cell | a 7.5305 · b 7.5305 · c 4.1263 Å · α 90° · β 90° · γ 120° |
| Transition | 5 K (−268 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Ce |
| Largest moment component | 1.22 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ce1 | Ce | 0.5857 | 0 | 0 | ||||
| Rh1 | Rh | 0 | 0 | 0 | ||||
| Pd1 | Pd | 0 | 0 | 0 | ||||
| Rh2 | Rh | 0.3333 | 0.6667 | 0.5 | ||||
| Pd2 | Pd | 0.3333 | 0.6667 | 0.5 | ||||
| Sn1 | Sn | 0.2488 | 0 | 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.
R. Tripathi et al. Phys. Rev. B (2022) · doi:10.1103/PhysRevB.106.064436
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.143_CeRh0.25Pd0.75Sn.mcif from MAGNDATA · entry page
sha256 of this copy: a70dd450863fede3eb2f1c0f362522af1eb02b99047c02170f16fb4a78790d83
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.143_CeRh0.25Pd0.75Sn.mcif.