Research/Sitter/MAGNDATA / 0.145_Co3TeO6.mcif
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| Magnetic group | C 2′/c BNS 15.87 |
| Point group | 2′/m |
| Parent space group | C 2/c No. 15 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 14.7832 · b 8.8396 · c 10.3428 Å · α 90° · β 95.03° · γ 90° |
| Transition | 21.1 K (−252 °C) |
| Magnetic ions | Co |
| Largest moment component | 2.2 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Co1 | Co | 0 | 0.3062 | 0.25 | −0.7 | 0 | 0.7 | 1.0324 |
| Co2 | Co | 0.8522 | 0.6398 | 0.2218 | 1.8 | 0.7 | 2.1 | 2.7344 |
| Co3 | Co | 0.5139 | 0.2983 | 0.07 | −2.2 | 0.6 | −1.9 | 2.842 |
| Co4 | Co | 0.6712 | 0.7102 | 0.0513 | 0.8 | 0.2 | 0.8 | 1.099 |
| Co5 | Co | 0.8091 | 0.6387 | 0.5665 | 2.1 | −0.9 | 1.9 | 2.8514 |
| Te1 | Te | 0 | 0.5 | 0 | ||||
| Te2 | Te | 0.6637 | 0.5089 | 0.3006 | ||||
| O1 | O | 0.9328 | 0.6607 | 0.5582 | ||||
| O2 | O | 0.5937 | 0.6511 | 0.2021 | ||||
| O3 | O | 0.5953 | 0.3682 | 0.2025 | ||||
| O4 | O | 0.7555 | 0.4814 | 0.6598 | ||||
| O5 | O | 0.9317 | 0.4924 | 0.3402 | ||||
| O6 | O | 0.5879 | 0.4826 | 0.4306 | ||||
| O7 | O | 0.9285 | 0.3584 | 0.5598 | ||||
| O8 | O | 0.7413 | 0.6721 | 0.4004 | ||||
| O9 | O | 0.7189 | 0.3482 | 0.3898 |
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. Ivanov et al. Materials Research Bulletin (2012) · doi:10.1016/j.materresbull.2011.10.003
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.145_Co3TeO6.mcif from MAGNDATA · entry page
sha256 of this copy: 69f50907307273adbed715530bfc22c5f7e08e503a3e0ed29225c2836ef405cd
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.145_Co3TeO6.mcif.