Research/Sitter/MAGNDATA / 1.1.68_CeAlGe.mcif
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| Magnetic group | Imm21′(α00)0s0s |
| Point group | mm21′ |
| Parent space group | I 41 m d No. 109 |
| Repeats every | 15.15 cells along a (not a whole number: that's what incommensurate means) |
| Propagation | [0.066 0 0] 1k |
| Cell | a 4.2572 · b 4.2572 · c 14.6452 Å · α 90° · β 90° · γ 90° |
| Transition | 4.4 K (−269 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Ce |
| Largest moment component | 1.45 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Al1_1 | Al | 0 | 0 | 0.18 | ||||
| Al1_2 | Al | 0 | 0.5 | 0.43 | ||||
| Ce1_1 | Ce | 0 | 0 | 0.59 | ||||
| Ce1_2 | Ce | 0 | 0.5 | 0.84 | ||||
| Ge1_1 | Ge | 0 | 0 | 0.01 | ||||
| Ge1_2 | Ge | 0 | 0.5 | 0.26 |
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.
P. Puphal et al. PHYSICAL REVIEW LETTERS (2020) · doi:10.1103/PhysRevLett.124.017202
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.68_CeAlGe.mcif from MAGNDATA · entry page
sha256 of this copy: 490638f75089c6cf233d7d0328e857bfccfb3618166ef913a89c2d3060876410
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.68_CeAlGe.mcif.