Research/Sitter/MAGNDATA / 1.1.158_(CH3NH3)Co0.5Ni0.5(HCOO)3.mcif
⬇ Download .mcif · Data (JSON)
| Magnetic group | Pn′ma′(00γ)0s0 |
| Point group | m′m′m |
| Parent space group | Pnma No. 62 |
| Repeats every | 8.01 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.1249] 1k |
| Cell | a 8.201 · b 11.5747 · c 8.1144 Å · α 90° · β 90° · γ 90° |
| Transition | 22.5 K (−251 °C) |
| Measured at | 2 K |
| Magnetic ions | Co, Ni |
| Largest moment component | 2.33 μB |
| Method | NSD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Co1 | Co | 0.5 | 0.5 | 1 | 0.71 | −0.6 | 2.33 | 2.5086 |
| Ni1 | Ni | 0.5 | 0.5 | 1 | 0.71 | −0.6 | 2.33 | 2.5086 |
| N1 | N | 0.5853 | 0.75 | 0.5299 | ||||
| C1 | C | 0.4118 | 0.75 | 0.4756 | ||||
| C2 | C | 0.2793 | 0.4706 | 0.7214 | ||||
| C3 | C | 0.5096 | 0.75 | 0.9449 | ||||
| O1 | O | 0.4034 | 0.4296 | 0.7869 | ||||
| O2 | O | 0.2263 | 0.441 | 0.5818 | ||||
| O3 | O | 0.5239 | 0.6548 | 0.8734 | ||||
| H1 | H | 0.5878 | 0.75 | 0.656 | ||||
| H2 | H | 0.646 | 0.8214 | 0.4878 | ||||
| H3 | H | 0.4079 | 0.75 | 0.3423 | ||||
| H4 | H | 0.3523 | 0.8259 | 0.5213 | ||||
| H5 | H | 0.2098 | 0.5362 | 0.7869 | ||||
| H6 | H | 0.4834 | 0.75 | 1.0777 |
Incommensurate: the moments are modulated; the picture evaluates each atom's Fourier series at its own phase.
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.
M. Geers et al. IUCrJ (2024) · doi:10.1107/S2052252524008583
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.158_(CH3NH3)Co0.5Ni0.5(HCOO)3.mcif from MAGNDATA · entry page
sha256 of this copy: 370e8f6b4e48d512de839a31a883a81e1d1bbda57f7b509f983aa0b53aa04361
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.158_(CH3NH3)Co0.5Ni0.5(HCOO)3.mcif.