Research/Sitter/MAGNDATA / 0.1144_Fe4Nb2O9.mcif
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| Magnetic group | P 1′ BNS 2.6 |
| Point group | 1′ |
| Parent space group | C 2/c No. 15 |
| Spins | noncoplanar · net moment 0 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 9.0861 · b 5.197 · c 14.234 Å · α 90° · β 91.29° · γ 90° |
| Transition | 87.5 K (−186 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Fe |
| Largest moment component | 5.43 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Nb1_1 | Nb | 0.001 | 0.9996 | 0.6428 | ||||
| Nb1_2 | Nb | 0.999 | 0.9996 | 0.8572 | ||||
| Fe1_1 | Fe | 0.832 | 0.4948 | 0.6887 | 3.57 | 1.1 | −0.86 | 3.8513 |
| Fe1_2 | Fe | 0.1706 | 0.5028 | 0.807 | −3.21 | −1.1 | 1.48 | 3.7307 |
| Fe2_1 | Fe | 0.8337 | 0.4915 | 0.484 | 4.37 | 0 | −1.94 | 4.821 |
| Fe2_2 | Fe | 0.1647 | 0.5094 | 0.0143 | −5.43 | 0 | 1.87 | 5.7826 |
| O1_1 | O | 0.845 | 0.821 | 0.0863 | ||||
| O1_2 | O | 0.155 | 0.821 | 0.4137 | ||||
| O2_1 | O | 0.672 | 0.355 | 0.0858 | ||||
| O2_2 | O | 0.328 | 0.355 | 0.4142 | ||||
| O3_1 | O | 0.986 | 0.328 | 0.0833 | ||||
| O3_2 | O | 0.014 | 0.328 | 0.4167 | ||||
| O4 | O | 0 | 0.722 | 0.25 | ||||
| O5_1 | O | 0.141 | 0.145 | 0.25 | ||||
| O5_2 | O | 0.859 | 0.145 | 0.25 |
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.
Raktim Datta et al. PHYSICAL REVIEW B (2025) · doi:10.1103/9tgw-l1nj
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.1144_Fe4Nb2O9.mcif from MAGNDATA · entry page
sha256 of this copy: 498cbabc7ded22167403fda11e8a8f6da2dd486c6177450a274b8f68736659b5
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1144_Fe4Nb2O9.mcif.