Research/Sitter/MAGNDATA / 1.303_Dy3Ru4Al12.mcif
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| Magnetic group | Cc 2/c BNS 15.90 |
| Parent space group | P 63/m m c No. 194 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [1/2 0 1/2] 1k |
| Cell | a 17.4808 · b 8.7404 · c 18.9964 Å · α 90° · β 90° · γ 120° |
| Transition | 7 K (−266 °C) |
| Measured at | 2.2 K |
| Magnetic ions | Dy |
| Largest moment component | 5.84 μB |
| Method | NSD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Dy1_1 | Dy | 0.0963 | 0.3851 | 0.125 | 1.65 | 3.3 | 5.84 | 6.5018 |
| Dy1_2 | Dy | 0.3074 | 0.8074 | 0.125 | −3.3 | −1.65 | 5.84 | 6.5018 |
| Ru1_1 | Ru | 0 | 0 | 0 | ||||
| Ru1_2 | Ru | 0 | 0 | 0.25 | ||||
| Ru2_1 | Ru | 0.25 | 0 | 0 | ||||
| Ru2_2 | Ru | 0 | 0.5 | 0 | ||||
| Ru2_3 | Ru | 0.25 | 0 | 0.25 | ||||
| Ru2_4 | Ru | 0 | 0.5 | 0.25 | ||||
| Al1_1 | Al | 0.7807 | 0.1226 | 0.125 | ||||
| Al1_2 | Al | 0.4387 | 0.4387 | 0.125 | ||||
| Al2_1 | Al | 0.4188 | 0.6751 | 0.0381 | ||||
| Al2_2 | Al | 0.1625 | 0.1625 | 0.0381 | ||||
| Al2_3 | Al | 0.5812 | 0.3249 | 0.2881 | ||||
| Al2_4 | Al | 0.8375 | 0.8375 | 0.2881 | ||||
| Al3_1 | Al | 0.1667 | 0.6667 | 0.2424 | ||||
| Al3_2 | Al | 0.3333 | 0.3333 | 0.4924 | ||||
| Al4 | Al | 0 | 0 | 0.125 |
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.
S. Gao et al. Phys. Rev. B (2019) · doi:10.1103/PhysRevB.100.241115
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.303_Dy3Ru4Al12.mcif from MAGNDATA · entry page
sha256 of this copy: 84b37b115bb364475238d86414ec446a1f89c220fc928026b056f5a4b9c6bb3d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.303_Dy3Ru4Al12.mcif.