Research/Sitter/MAGNDATA / 1.0.45_Ba3CoSb2O9.mcif
⬇ Download .mcif · Data (JSON)
| Magnetic group | P 6 2 m BNS 189.221 |
| Parent space group | P 63/m m c No. 194 |
| Spins | coplanar · net moment 0 μB per cell |
| Propagation | [1/3 1/3 0] 1k |
| Cell | a 17.5239 · b 17.5239 · c 14.4283 Å · α 90° · β 90° · γ 120° |
| Transition | 3.8 K (−269 °C) |
| Measured at | 1.7 K |
| Magnetic ions | Co |
| Largest moment component | 1 μB |
| Method | NSD unpolarized and polarized |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ba1_1 | Ba | 0 | 0 | 0.25 | ||||
| Ba1_2 | Ba | 0 | 0 | 0.75 | ||||
| Ba2_1 | Ba | 0.1111 | 0.2222 | 0.9112 | ||||
| Ba2_2 | Ba | 0.2222 | 0.1111 | 0.4112 | ||||
| Ba2_3 | Ba | 0.1111 | 0.8889 | 0.9112 | ||||
| Co1 | Co | 0 | 0 | 0 | 1 | 1 | 0 | 1 |
| Sb1_1 | Sb | 0.1111 | 0.2222 | 0.1518 | ||||
| Sb1_2 | Sb | 0.2222 | 0.1111 | 0.6518 | ||||
| Sb1_3 | Sb | 0.1111 | 0.8889 | 0.1518 | ||||
| O1_1 | O | 0.1609 | 0.3219 | 0.25 | ||||
| O1_2 | O | 0.1609 | 0.8391 | 0.25 | ||||
| O1_3 | O | 0.8391 | 0.6781 | 0.75 | ||||
| O1_4 | O | 0.8391 | 0.1609 | 0.75 | ||||
| O2_1 | O | 0.0566 | 0.1131 | 0.4157 | ||||
| O2_2 | O | 0.0566 | 0.9434 | 0.4157 | ||||
| O2_3 | O | 0.9434 | 0.8869 | 0.9157 | ||||
| O2_4 | O | 0.9434 | 0.0566 | 0.9157 |
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.
J. Ma et al. PHYSICAL REVIEW LETTERS (2016) · doi:10.1103/PhysRevLett.116.087201
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.0.45_Ba3CoSb2O9.mcif from MAGNDATA · entry page
sha256 of this copy: 5f67d93f397c1f705b0648cd1c969a62019da5d690d9b93d05fd4443f8445f0f
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.0.45_Ba3CoSb2O9.mcif.