Research/Sitter/MAGNDATA / 1.820_Ba4TbRu3O12.mcif
⬇ Download .mcif · Data (JSON)
| Magnetic group | Cc m BNS 8.35 |
| Point group | m1′ |
| Parent space group | R 3 m No. 166 |
| Spins | collinear · net moment 0 μB per cell |
| Propagation | [0 0 3/2] 1k |
| Cell | a 5.8144 · b 5.8144 · c 57.9296 Å · α 90° · β 90° · γ 120° |
| Transition | 24 K (−249 °C) |
| Measured at | 2.5 K |
| Magnetic ions | Ru, Tb |
| Largest moment component | 5.78 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Ba1_1 | Ba | 0 | 0 | 0.0649 | ||||
| Ba1_2 | Ba | 0 | 0 | 0.9351 | ||||
| Ba2_1 | Ba | 0 | 0 | 0.1429 | ||||
| Ba2_2 | Ba | 0 | 0 | 0.857 | ||||
| Tb1 | Tb | 0 | 0 | 0 | 5.78 | 0 | 0 | 5.78 |
| Ru1 | Ru | 0 | 0 | 0.25 | −0.96 | 0 | 0 | 0.96 |
| Ru2_1 | Ru | 0 | 0 | 0.2066 | 0.96 | 0 | 0 | 0.96 |
| Ru2_2 | Ru | 0 | 0 | 0.7934 | −0.96 | 0 | 0 | 0.96 |
| O1_1 | O | 0.489 | 0.511 | 0.0617 | ||||
| O1_2 | O | 0.489 | 0.978 | 0.0617 | ||||
| O1_3 | O | 0.511 | 0.489 | 0.9383 | ||||
| O1_4 | O | 0.511 | 0.022 | 0.9383 | ||||
| O2_1 | O | 0.4952 | 0.5048 | 0.1456 | ||||
| O2_2 | O | 0.4952 | 0.9904 | 0.1456 | ||||
| O2_3 | O | 0.5048 | 0.4952 | 0.8545 | ||||
| O2_4 | O | 0.5048 | 0.0096 | 0.8545 |
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.
Y. Shimoda et al. Chem. Mater. (2008) · doi:10.1021/cm800708g
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.820_Ba4TbRu3O12.mcif from MAGNDATA · entry page
sha256 of this copy: ef929a868e0c1c3e1f5f7d48d8d8dce2cb58c7a74e5e55a0157de828ddc10788
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.820_Ba4TbRu3O12.mcif.