Research/Sitter/MAGNDATA / 1.800_NiO.mcif
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| Magnetic group | Cc 2/c BNS 15.90 |
| Point group | 2/m1′ |
| Parent space group | F m 3 m No. 225 |
| Spins | collinear · net moment 0 μB per cell |
| Propagation | [1/2 1/2 1/2] 1k |
| Cell | a 5.10964 · b 2.95005 · c 5.89292 Å · α 90° · β 125.314° · γ 90° |
| Transition | 525 K (252 °C) |
| Measured at | 1.8 K |
| Magnetic ions | Ni |
| Largest moment component | 2.1283 μB |
| Method | A different 3k rhombohedral model with MSG RI-3c (see entry #3.28) can equally well fit the diffraction data, and with similar value of m. The present model is however considered more probable as the one corresponding to the real system. See the discussion in the paper for further details. |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ni1 | Ni | 0 | 0 | 0 | 2.1283 | 0 | 0.76 | 1.7992 |
| O1 | O | 0 | 0.5 | 0.75 |
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.
V. Pomjakushin et al. Acta Cryst. B (2024) · doi:10.1107/S205252062400756X
Cite the original paper and MAGNDATA, not this mirror.
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sha256 of this copy: 221265d2e57e00c42d68043e2da6d6e9df0959e0359dbecb8201ad47a5f72edc
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.800_NiO.mcif.