Research/Sitter/MAGNDATA / 1.1.130_Ce5TeO8.mcif
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| Magnetic group | P43(0,0,γ)0 |
| Point group | 4 |
| Parent space group | P 43 3 2 No. 212 |
| Repeats every | 11.64 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.0859] 1k |
| Cell | a 8.54975 · b 8.54975 · c 8.54975 Å · α 90° · β 90° · γ 90° |
| Transition | 45 K (−228 °C) |
| Measured at | 30 K |
| Magnetic ions | Co |
| Largest moment component | 126 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Co1_1 | Co | 0.0006 | −0.0006 | 0.0006 | 0 | 0 | −1.25 | 1.25 |
| Co1_2 | Co | 0.5006 | 0.0006 | 0.4994 | 0 | 0 | −1.25 | 1.25 |
| Co2_1 | Co | 0.125 | 0.137 | 0.387 | 0 | 0 | 1.56 | 1.56 |
| Co2_2 | Co | 0.625 | 0.863 | 0.113 | 0 | 0 | 1.56 | 1.56 |
| Co2_3 | Co | 0.863 | 0.613 | 0.125 | 0 | 0 | 1.56 | 1.56 |
| Te_1 | Te | 0.625 | 0.375 | 0.625 | ||||
| O1_1 | O | 0.3789 | 0.6211 | 0.3789 | ||||
| O1_2 | O | 0.8789 | 0.3789 | 0.1211 | ||||
| O2_1 | O | 0.3518 | 0.6268 | 0.8659 | ||||
| O2_2 | O | 0.8518 | 0.3732 | 0.6341 | ||||
| O2_3 | O | 0.8659 | 0.6482 | 0.3732 | ||||
| O2_4 | O | 0.3659 | 0.3518 | 0.1268 | ||||
| O2_5 | O | 0.3732 | 0.1341 | 0.3518 | ||||
| O2_6 | O | 0.8732 | 0.8659 | 0.1482 |
Incommensurate: the moments are modulated; the picture evaluates each atom's Fourier series at its own phase.
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. Podchezertsev et al. Inorg. Chem. (2021) · doi:10.1021/acs.inorgchem.1c01131
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.130_Ce5TeO8.mcif from MAGNDATA · entry page
sha256 of this copy: d8e8206d4c40709ca6b56c775e87cd5c60c174ac0c436bfcd407a7866bb7f6b4
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.130_Ce5TeO8.mcif.