Research/Sitter/MAGNDATA / 1.1.63_GdMn2O5.mcif
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| Magnetic group | Xb21m1′(00γ)000s |
| Point group | mm21′ |
| Parent space group | P b a m No. 55 |
| Repeats every | 10 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.1] 1k |
| Cell | a 14.7062 · b 8.5371 · c 5.6807 Å · α 90° · β 90° · γ 90° |
| Transition | 40 K (−233 °C) |
| Measured at | 33.5 K |
| Magnetic ions | Gd, Mn |
| Largest moment component | 2.73 μB |
| Method | NSD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Gd1_1 | Gd | 0.0695 | 0.172 | 0 | ||||
| Gd1_2 | Gd | 0.3195 | 0.328 | 0 | ||||
| Mn1 | Mn | 0 | 0.5 | 0.256 | ||||
| Mn2_1 | Mn | 0.2055 | 0.349 | 0.5 | ||||
| Mn2_2 | Mn | 0.2945 | 0.651 | 0.5 |
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.
J. Sheng et al. PHYSICAL REVIEW B (2019) · doi:10.1103/PhysRevB.99.094429
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.63_GdMn2O5.mcif from MAGNDATA · entry page
sha256 of this copy: 8a87c8d0e077d7f179846adb220c5a0fb1aacb62db51f9a466c7eaef3b84f026
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.63_GdMn2O5.mcif.