Research/Sitter/MAGNDATA / 1.443_Gd2BaCuO5.mcif
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| Magnetic group | Pa c a 21 BNS 29.104 |
| Point group | mm21′ |
| Parent space group | P n m a No. 62 |
| Spins | coplanar · net moment 0 μB per cell |
| Propagation | [0 0 1/2] 1k |
| Cell | a 12.2185 · b 5.6779 · c 14.329 Å · α 90° · β 90° · γ 90° |
| Transition | 6 K (−267 °C) |
| Measured at | 1.3 K |
| Magnetic ions | Cu, Gd |
| Largest moment component | 6.86 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Gd1_1 | Gd | 0.2886 | 0.25 | 0.0578 | −6.75 | 0 | −1.295 | 6.8731 |
| Gd1_2 | Gd | 0.2114 | 0.75 | 0.3078 | −0.347 | 0 | 6.86 | 6.8688 |
| Gd2_1 | Gd | 0.0738 | 0.25 | 0.1908 | 6.17 | 0 | 2.38 | 6.6131 |
| Gd2_2 | Gd | 0.4262 | 0.75 | 0.4408 | −2.56 | 0 | −6.1 | 6.6154 |
| Cu_1 | Cu | 0.6595 | 0.25 | 0.3564 | 0.272 | 0 | −0.969 | 1.0065 |
| Cu_2 | Cu | 0.8405 | 0.75 | 0.6065 | −0.33 | 0 | −0.95 | 1.0057 |
| Ba1_1 | Ba | 0.9056 | 0.25 | 0.4657 | ||||
| Ba1_2 | Ba | 0.5944 | 0.75 | 0.7157 | ||||
| O1_1 | O | 0.4325 | 0.988 | 0.0853 | ||||
| O1_2 | O | 0.0675 | 0.012 | 0.3352 | ||||
| O2_1 | O | 0.2251 | 0.505 | 0.1725 | ||||
| O2_2 | O | 0.2749 | 0.495 | 0.4225 | ||||
| O3_1 | O | 0.094 | 0.25 | 0.0345 | ||||
| O3_2 | O | 0.406 | 0.75 | 0.2845 |
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.
⬇ 1.443_Gd2BaCuO5.mcif from MAGNDATA · entry page
sha256 of this copy: bef849ec8f65255f2c4e455de28834a82bda7c128630829fb9e0d54256639609
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.443_Gd2BaCuO5.mcif.