Research/Sitter/MAGNDATA / 1.115_Dy3Ru4Al12.mcif
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| Magnetic group | Cc 2/c BNS 15.90 |
| Point group | 2/m1′ |
| 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 15.1388 · b 8.7404 · c 18.9965 Å · α 90° · β 90° · γ 90° |
| Transition | 7 K (−266 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Dy |
| Largest moment component | 0.5 μB |
| Method | NSD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Dy1_1 | Dy | 0.0963 | 0.2888 | 0.125 | 0.01 | −0.18 | 0.5 | 0.5315 |
| Dy1_2 | Dy | 0.3074 | 0.5 | 0.625 | −0.5 | 0 | −0.5 | 0.7071 |
| Ru1_1 | Ru | 0.25 | 0.75 | 0 | ||||
| Ru1_2 | Ru | 0 | 0.5 | 0 | ||||
| Ru1_3 | Ru | 0.25 | 0.75 | 0.25 | ||||
| Ru1_4 | Ru | 0 | 0.5 | 0.25 | ||||
| Ru2_1 | Ru | 0 | 0 | 0 | ||||
| Ru2_2 | Ru | 0 | 0 | 0.25 | ||||
| Al1_1 | Al | −0.3376 | 0.5 | 0.5381 | ||||
| Al1_2 | Al | 0.1624 | 0 | 0.2119 | ||||
| Al1_3 | Al | 0.4188 | −0.2563 | 0.5381 | ||||
| Al1_4 | Al | −0.0812 | 0.7563 | 0.2119 | ||||
| Al2_1 | Al | −0.2193 | 0.342 | 0.625 | ||||
| Al2_2 | Al | −0.0614 | 0.5 | 0.125 | ||||
| Al3_1 | Al | −0.1667 | 0.5 | 0.4924 | ||||
| Al3_2 | Al | −0.1667 | 0.5 | 0.7576 | ||||
| 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.
D.I. Gorbunov et al. PHYSICAL REVIEW B (2014) · doi:10.1103/PhysRevB.90.094405
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.115_Dy3Ru4Al12.mcif from MAGNDATA · entry page
sha256 of this copy: c2643eb4f4139650850f9c313baca9a56daa4b38a7432f801a1b60adc40df45c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.115_Dy3Ru4Al12.mcif.