Research/Sitter/MAGNDATA / 1.1.12_MnWO4.mcif
⬇ Download .mcif · Data (JSON)
| Magnetic group | X2/c1′(α0γ)0ss |
| Point group | 2/m1′ |
| Parent space group | P 2/c No. 13 |
| Repeats every | 2.19 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [-0.214 0 0.457] 1k |
| Cell | a 4.8228 · b 11.5106 · c 5.0013 Å · α 90° · β 91.1025° · γ 90° |
| Transition | 13.5 K (−260 °C) |
| Measured at | 13 K |
| Magnetic ions | Mn |
| Largest moment component | 1.46 μB |
| Method | Phase AF3 |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Mn1 | Mn | 0.5 | 0.3422 | 0.25 | ||||
| W1 | W | 0 | 0.0898 | 0.25 | ||||
| O1 | O | 0.2106 | 0.0512 | 0.9438 | ||||
| O2 | O | 0.2503 | 0.1872 | 0.3943 |
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.
I. Urcelay-Olabarria et al. PHYSICAL REVIEW B (2013) · doi:10.1103/PhysRevB.87.014419
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.12_MnWO4.mcif from MAGNDATA · entry page
sha256 of this copy: cf27bfe636d3d800d3691284efebdd6711b4ceb30aa05e7768a9995a5fe8c0e2
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.12_MnWO4.mcif.