Research/Sitter/MAGNDATA / 1.1.79_Pb2MnWO6.mcif
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| Magnetic group | Pmc211′(α00)0s0s |
| Point group | mm21′ |
| Parent space group | P m c 21 No. 26 |
| Repeats every | 4.35 cells along a (not a whole number: that's what incommensurate means) |
| Propagation | [0.23 0 0] 1k |
| Cell | a 8.0206 · b 5.7813 · c 11.6316 Å · α 90° · β 90° · γ 90° |
| Transition | 9 K (−264 °C) |
| Measured at | 7.9 K |
| Magnetic ions | Mn |
| Largest moment component | 2.11 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Pb1 | Pb | 0.7628 | 0.9746 | 0.8653 | ||||
| Pb2 | Pb | 0.7462 | 0.5477 | 0.5786 | ||||
| W1 | W | 0 | 0.522 | 0.8644 | ||||
| W2 | W | 0.5 | 0.001 | 0.6117 | ||||
| Mn1 | Mn | 0.5 | 0.492 | 0.8646 | ||||
| Mn2 | Mn | 0 | 0.998 | 0.1027 | ||||
| O1 | O | 0 | 0.724 | 0.73 | ||||
| O2 | O | 0 | 0.311 | 0.973 | ||||
| O3 | O | 0.5 | 0.767 | 0.7103 | ||||
| O4 | O | 0.5 | 0.222 | 0.721 | ||||
| O5 | O | 0 | 0.249 | 0.7442 | ||||
| O6 | O | 0.5 | 0.209 | 0.477 | ||||
| O7 | O | 0.7384 | 0.0361 | 0.5956 | ||||
| O8 | O | 0.5 | 0.294 | 0.9958 | ||||
| O9 | O | 0.7667 | 0.52 | 0.8655 | ||||
| O10 | O | 0 | 0.786 | 0.9568 |
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.
F. Orlandi et al. J. Mater. Chem. C (2014) · doi:10.1039/c4tc01450b
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.79_Pb2MnWO6.mcif from MAGNDATA · entry page
sha256 of this copy: 524f3bffde91407c4f8cce47fb6202419a28e14980c7ff161d0937069e0ee7a4
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.79_Pb2MnWO6.mcif.