Research/Sitter/MAGNDATA / 1.1.53_YBaCuFeO5.mcif
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| Magnetic group | P4221′(1/21/2γ)q00s |
| Point group | 4221′ |
| Parent space group | P 4/m m m No. 123 |
| Repeats every | 2 cells along a (not a whole number: that's what incommensurate means) |
| Propagation | [0.5 0.5 0.4122] 1k |
| Cell | a 3.8674 · b 3.8674 · c 7.6317 Å · α 90° · β 90° · γ 90° |
| Transition | 175 K (−98 °C) |
| Measured at | 3.5 K |
| Magnetic ions | Cu, Fe |
| Largest moment component | 2.95 μB |
| Method | NSD and NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Y1_1 | Y | 0 | 0 | 0.5 | ||||
| Ba1_1 | Ba | 0 | 0 | 0 | ||||
| Cu1_1 | Cu | 0.5 | 0.5 | 0.2833 | ||||
| Fe1_1 | Fe | 0.5 | 0.5 | 0.2546 | ||||
| O1_1 | O | 0.5 | 0.5 | 0 | ||||
| O2_1 | O | 0 | 0.5 | 0.6847 |
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.
Y.-C. Lai et al. J. Phys.: Condens. Matter (2017) · doi:10.1088/1361-648X/aa5708
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.53_YBaCuFeO5.mcif from MAGNDATA · entry page
sha256 of this copy: 331c29d0befc4e66cf25640ed69b6d7f13a4d87e4f17cdc02ba2eda6792ed420
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.53_YBaCuFeO5.mcif.