Research/Sitter/MAGNDATA / 0.127_Dy3Al5O12.mcif
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| Magnetic group | I a 3d′ BNS 230.148 |
| Point group | m3m′ |
| Parent space group | I a 3d No. 230 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 12.376 · b 12.376 · c 12.376 Å · α 90° · β 90° · γ 90° |
| Transition | 2.49 K (−271 °C) |
| Magnetic ions | Dy |
| Largest moment component | 9 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Dy1 | Dy | 0.125 | 0 | 0.25 | −9 | 0 | 0 | 9 |
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.
J.M. Hastings et al. Phys. Rev. (1965) · doi:10.1103/PhysRev.138.A176
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.127_Dy3Al5O12.mcif from MAGNDATA · entry page
sha256 of this copy: f5b0c8c4489a57cb5ec8f83079fbafaa40067aa9f5d55722222187786db64d4b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.127_Dy3Al5O12.mcif.