Research/Sitter/MAGNDATA / 1.1.92_Gd2BaCuO5.mcif
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| Magnetic group | P21ma1′(0,0,γ)0s0s |
| Point group | mm21′ |
| Parent space group | P n m a No. 62 |
| Repeats every | 2.25 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.4449] 1k |
| Cell | a 12.2282 · b 5.67992 · c 7.16183 Å · α 90° · β 90° · γ 90° |
| Transition | 11.8 K (−261 °C) |
| Measured at | 9.8 K |
| Magnetic ions | Cu, Ho |
| Largest moment component | 7.11 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Gd1_1 | Ho | 0.2886 | 0.25 | 0.1156 | ||||
| Gd1_2 | Ho | 0.7114 | 0.75 | 0.8844 | ||||
| Gd2_1 | Ho | 0.0738 | 0.25 | 0.3954 | ||||
| Gd2_2 | Ho | −0.0738 | 0.75 | 0.6046 | ||||
| Cu_1 | Cu | 0.6592 | 0.25 | 0.7129 | ||||
| Cu_2 | Cu | 0.3408 | 0.75 | 0.2871 | ||||
| Ba1_1 | Ba | 0.9056 | 0.25 | 0.9313 | ||||
| Ba1_2 | Ba | 0.5944 | 0.75 | 0.4313 | ||||
| O1_1 | O | 0.4325 | 0.988 | 0.1705 | ||||
| O1_2 | O | 0.0675 | 0.012 | 0.6705 | ||||
| O2_1 | O | 0.2251 | 0.505 | 0.345 | ||||
| O2_2 | O | 0.2749 | 0.495 | 0.845 | ||||
| O3_1 | O | 0.094 | 0.25 | 0.069 | ||||
| O3_2 | O | 0.406 | 0.75 | 0.569 |
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.
P. Yanda et al. PHYSICAL REVIEW RESEARCH (2020) · doi:10.1103/PhysRevResearch.2.023271
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.92_Gd2BaCuO5.mcif from MAGNDATA · entry page
sha256 of this copy: b3e0bcbdfd8de06fdf27846a0f629c06afc28cb04ff4a328b14f268430d8f622
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.92_Gd2BaCuO5.mcif.