Research/Sitter/MAGNDATA / 1.1.16_CeRhIn5.mcif
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| Magnetic group | P4221′(1/2,1/2,γ)q00s |
| Point group | 4221′ |
| Parent space group | P 4/m m m No. 123 |
| Repeats every | 2 cells along a (not a whole number: that's what incommensurate means) |
| Propagation | [0.5 0.5 0.297] 1k |
| Cell | a 4.6551 · b 4.6551 · c 7.5426 Å · α 90° · β 90° · γ 90° |
| Transition | 3.8 K (−269 °C) |
| Measured at | 1.4 K |
| Magnetic ions | Ce |
| Largest moment component | 0.75 μB |
| Method | NSD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ce1 | Ce | 0 | 0 | 0 | ||||
| Rh1 | Rh | 0 | 0 | 0.5 | ||||
| In1 | In | 0.5 | 0.5 | 0 | ||||
| In2 | In | 0 | 0.5 | 0.3059 |
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.
W. Bao et al. PHYSICAL REVIEW B (2000) · doi:10.1103/PhysRevB.62.R14621
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.16_CeRhIn5.mcif from MAGNDATA · entry page
sha256 of this copy: 082055e355f242ed0e34e3b1e8f0ed028672037fef1949100a217febb16c41b7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.16_CeRhIn5.mcif.