Research/Sitter/MAGNDATA / 0.521_DyCoO3.mcif
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| Magnetic group | P n′ m′ a′ BNS 62.449 |
| Parent space group | P b n m No. 62 |
| Spins | coplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 5.1642 · b 5.4165 · c 7.3802 Å · α 90° · β 90° · γ 90° |
| Transition | 3.6 K (−270 °C) |
| Measured at | 0.25 K |
| Magnetic ions | Dy |
| Largest moment component | 8 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Dy1 | Dy | −0.0157 | 0.0662 | 0.25 | −4.3 | 8 | 0 | 9.0824 |
| Co1 | Co | 0.5 | 0 | 0 | ||||
| O1 | O | 0.4051 | −0.0193 | 0.25 | ||||
| O2 | O | 0.6994 | 0.3028 | 0.0448 |
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.
K. Knizek et al. Solid State Sciences (2014) · doi:10.1016/j.solidstatesciences.2013.12.001
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.521_DyCoO3.mcif from MAGNDATA · entry page
sha256 of this copy: cc0e3eeafd6dde1c2ca6d0b0f152f1d8c7dea270ece321dfa1dd82e1633164ec
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.521_DyCoO3.mcif.