Research/Sitter/MAGNDATA / 1.1.154_CePtAl4Ge2.mcif
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| Magnetic group | B2/m1′(α,β,0)0ss |
| Point group | 2/m1′ |
| Parent space group | R3m No. 166 |
| Repeats every | 1.05 cells along b (not a whole number: that's what incommensurate means) |
| Propagation | [0.86667 -0.95667 0] 1k |
| Cell | a 21.26216 · b 10.83481 · c 4.18243 Å · α 90° · β 90° · γ 19.39862° |
| Transition | 2.3 K (−271 °C) |
| Measured at | 0.07 K |
| Magnetic ions | Ce |
| Largest moment component | 3.871 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Al1 | Al | −0.0806 | −0.0806 | 0 | ||||
| Al2 | Al | 0.3064 | 0.3064 | 0 | ||||
| Ce1 | Ce | 0 | 0.5 | 0.5 | ||||
| Ge1 | Ge | 0.2237 | 0.2237 | 0 | ||||
| Pt1 | Pt | 0 | 0 | 0 |
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.
S. Shin et al. PHYSICAL REVIEW B (2020) · doi:10.1103/PhysRevB.101.224421
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.154_CePtAl4Ge2.mcif from MAGNDATA · entry page
sha256 of this copy: 7660559b052758f69fefe17b94dd7f813f4bbfaf900102863292ca0bb35905e4
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.154_CePtAl4Ge2.mcif.