Research/Sitter/MAGNDATA / 2.85_Ho2BaCuO5.mcif
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| Magnetic group | P 21′/c BNS 14.77 |
| Point group | 2′/m |
| Parent space group | P n m a No. 62 |
| Spins | coplanar · net moment 0 μB per cell |
| Propagation | [0 1/2 0] · [0 0 0] 2k |
| Cell | a 12.1776 · b 11.3235 · c 7.1228 Å · α 90° · β 90° · γ 90° |
| Transition | 8 K (−265 °C) |
| Measured at | 2.3 K |
| Magnetic ions | Cu, Ho |
| Largest moment component | 8.46 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ho1_1 | Ho | 0.2868 | 0.125 | 0.1164 | 7.17 | 0 | 0.82 | 7.2167 |
| Ho1_2 | Ho | 0.2868 | 0.625 | 0.1164 | −2.59 | 0 | 2.86 | 3.8585 |
| Ho2_1 | Ho | 0.0745 | 0.125 | 0.3957 | 1.05 | 0 | −8.46 | 8.5249 |
| Ho2_2 | Ho | 0.0745 | 0.625 | 0.3957 | 1.17 | 0 | −8.32 | 8.4019 |
| Cu1_1 | Cu | 0.6581 | 0.125 | 0.7077 | −0.77 | 0 | 0.65 | 1.0077 |
| Cu1_2 | Cu | 0.6581 | 0.625 | 0.7077 | 0.69 | 0 | 0.17 | 0.7106 |
| Ba1_1 | Ba | 0.903 | 0.125 | 0.932 | ||||
| Ba1_2 | Ba | 0.903 | 0.625 | 0.932 | ||||
| O1_1 | O | 0.435 | 0.9991 | 0.1646 | ||||
| O1_2 | O | 0.435 | 0.4991 | 0.1646 | ||||
| O1_3 | O | 0.935 | 0.2509 | 0.3354 | ||||
| O1_4 | O | 0.935 | 0.7509 | 0.3354 | ||||
| O2_1 | O | 0.2275 | 0.7534 | 0.351 | ||||
| O2_2 | O | 0.2275 | 0.2534 | 0.351 | ||||
| O2_3 | O | 0.7275 | 0.4966 | 0.149 | ||||
| O2_4 | O | 0.7275 | 0.9966 | 0.149 | ||||
| O3_1 | O | 0.102 | 0.125 | 0.085 | ||||
| O3_2 | O | 0.102 | 0.625 | 0.085 |
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 B (2021) · doi:10.1103/PhysRevB.104.144401
Cite the original paper and MAGNDATA, not this mirror.
⬇ 2.85_Ho2BaCuO5.mcif from MAGNDATA · entry page
sha256 of this copy: 0bdaaa3d2d27cf4f1ce08e1af10088b49c49099af7a7e088235b44b19352ef0b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.85_Ho2BaCuO5.mcif.