Research/Sitter/MAGNDATA / 0.250_(NH2(CH3)2)(FeCo(HCOO)6).mcif
⬇ Download .mcif · Data (JSON)
| Magnetic group | C 2′/c′ BNS 15.89 |
| Point group | 2′/m′ |
| Parent space group | P 3 c 1 No. 163 |
| Spins | noncoplanar · net moment 3.544 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 8.2501 · b 8.2501 · c 13.7188 Å · α 90° · β 90° · γ 120° |
| Transition | 32 K (−241 °C) |
| Measured at | 2 K |
| Magnetic ions | Co, Fe |
| Largest moment component | 4.6 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Co1 | Co | 0.3333 | 0.6667 | 0.25 | −2.2 | −2.2 | −1 | 2.4166 |
| Fe1 | Fe | 0 | 0 | 0 | 3.2 | 4.6 | 1.5 | 4.3509 |
| O1_1 | O | 0.1166 | 0.6564 | 0.1681 | ||||
| O1_2 | O | 0.3436 | 0.4602 | 0.1681 | ||||
| O1_3 | O | 0.5398 | 0.8834 | 0.1681 | ||||
| O2_1 | O | 0.9868 | 0.7911 | 0.0829 | ||||
| O2_2 | O | 0.2089 | 0.1956 | 0.0829 | ||||
| O2_3 | O | 0.8044 | 0.0132 | 0.0829 | ||||
| C1_1 | C | 0.1268 | 0.7898 | 0.1202 | ||||
| C1_2 | C | 0.2102 | 0.3369 | 0.1202 | ||||
| C1_3 | C | 0.6631 | 0.8732 | 0.1202 | ||||
| H1_1 | H | 0.2447 | 0.8952 | 0.1112 | ||||
| H1_2 | H | 0.1048 | 0.3495 | 0.1112 | ||||
| H1_3 | H | 0.6505 | 0.7553 | 0.1112 | ||||
| C2 | C | 0.3333 | 0.6667 | 0.8442 | ||||
| N1_1 | N | 0.7224 | 0.4447 | 0.25 | ||||
| N1_2 | N | 0.7224 | 0.2778 | 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.
L. Mazzuca et al. Inorg. Chem. (2017) · doi:10.1021/acs.inorgchem.6b01866
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.250_(NH2(CH3)2)(FeCo(HCOO)6).mcif from MAGNDATA · entry page
sha256 of this copy: e0833a90c006261bcade9e5e24fc04e720d3d0d156019f3af3d28275acdc2c01
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.250_(NH2(CH3)2)(FeCo(HCOO)6).mcif.