Research/Sitter/MAGNDATA / 0.440_SrCuTe2O6.mcif
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| Magnetic group | P 41 3 2 BNS 213.63 |
| Parent space group | P 41 3 2 No. 213 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 12.4321 · b 12.4321 · c 12.4321 Å · α 90° · β 90° · γ 90° |
| Transition | 5.25 K (−268 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Cu |
| Largest moment component | 0.37 μB |
| Method | NPD and NSD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Te1 | Te | 0.3379 | 0.9192 | 0.0589 | ||||
| Sr1 | Sr | 0.0536 | 0.0536 | 0.0536 | ||||
| Sr2 | Sr | 0.875 | 0.875 | 0.875 | ||||
| Cu1 | Cu | 0.476 | 0.875 | 0.274 | 0.37 | 0 | −0.37 | 0.5233 |
| O1 | O | 0.6702 | 0.1271 | 0.1795 | ||||
| O2 | O | 0.4391 | 0.0163 | 0.2271 | ||||
| O3 | O | 0.222 | 0.9766 | 0.1297 |
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. Saeaun et al. PHYSICAL REVIEW B (2020) · doi:10.1103/PhysRevB.102.134407
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.440_SrCuTe2O6.mcif from MAGNDATA · entry page
sha256 of this copy: 084e3ae4a53eafd80375b0ec61355aefb57aef0e5b8238978fd29d6078bd0b93
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.440_SrCuTe2O6.mcif.