Research/Sitter/MAGNDATA / 0.170_U3P4.mcif
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| Magnetic group | R 3c′ BNS 161.71 |
| Point group | 3m′ |
| Parent space group | I 43d No. 220 |
| Spins | noncoplanar · net moment 17.321 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 8.212 · b 8.212 · c 8.212 Å · α 90° · β 90° · γ 90° |
| Transition | 140 K (−133 °C) |
| Magnetic ions | U |
| Largest moment component | 1.1 μB |
| Method | NSD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| U1 | U | 0.375 | 0 | 0.25 | 1.1 | 0.7 | 0.7 | 1.4799 |
| P1_1 | P | 0.083 | 0.083 | 0.083 | ||||
| P1_2 | P | 0.417 | 0.917 | 0.583 |
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. Burlet et al. Solid State Communications (1981) · doi:10.1016/0038-1098(81)90449-X
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.170_U3P4.mcif from MAGNDATA · entry page
sha256 of this copy: 4b52c4d77836f6949531bd3d2da6570af0ddcfa3decdd02028972ceaf15e86a0
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.170_U3P4.mcif.