Research/Sitter/MAGNDATA / 1.1.42_YbCo2Si2.mcif
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| Magnetic group | I112/m1′(αβ0)000ss |
| Point group | 2/m1′ |
| Parent space group | I 4/m m m No. 139 |
| Repeats every | 1.33 cells along a (not a whole number: that's what incommensurate means) |
| Propagation | [-0.75 0.086 0] 1k |
| Cell | a 3.8533 · b 3.8533 · c 9.6777 Å · α 90° · β 90° · γ 90° |
| Transition | 1.4 K (−272 °C) |
| Measured at | 1.1 K |
| Magnetic ions | Yb |
| Largest moment component | 1.12 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Yb1 | Yb | 0 | 0 | 0 | ||||
| Co1 | Co | 0 | 0.5 | 0.25 | ||||
| Si1 | Si | 0 | 0 | 0.38 |
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.
N. Mufti et al. PHYSICAL REVIEW B (2016) · doi:10.1103/PhysRevB.94.045116
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.42_YbCo2Si2.mcif from MAGNDATA · entry page
sha256 of this copy: 3229f39cff0aca738bc040660a7051413e66f08b64f3d781c2ab74928b57d7dc
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.42_YbCo2Si2.mcif.