Research/Sitter/MAGNDATA / 1.1.127_(Lu0.9Mn0.1)MnO3.mcif
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| Magnetic group | Pnma1′(α,0,0)0sss |
| Point group | mmm1′ |
| Parent space group | P n m a No. 62 |
| Repeats every | 2.28 cells along a (not a whole number: that's what incommensurate means) |
| Propagation | [0.438 0 0] 1k |
| Cell | a 5.7 · b 7.3087 · c 5.1892 Å · α 90° · β 90° · γ 90° |
| Transition | 36 K (−237 °C) |
| Measured at | 2 K |
| Magnetic ions | Mn |
| Largest moment component | 2.84 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Lu1 | Lu | 0.0847 | 0.25 | −0.0188 | ||||
| Mn1 | Mn | 0.0847 | 0.25 | −0.0188 | ||||
| Mn2 | Mn | 0 | 0 | 0.5 | ||||
| O1 | O | 0.4573 | 0.25 | 0.1179 | ||||
| O2 | O | 0.3254 | 0.0563 | 0.6963 |
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.
L. Zhang et al. Inorg. Chem. (2018) · doi:10.1021/acs.inorgchem.8b01470
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.127_(Lu0.9Mn0.1)MnO3.mcif from MAGNDATA · entry page
sha256 of this copy: cc01d022b8a1fa143a3fa765e885bd52788fb47c049b17ea0d396a9cd5159904
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.127_(Lu0.9Mn0.1)MnO3.mcif.