Research/Sitter/MAGNDATA / 1.1.64_K2MnS2.mcif
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| Magnetic group | Ic2m1′(α,0,0)000s |
| Point group | m2m1′ |
| Parent space group | Ibam No. 72 |
| Repeats every | 2.38 cells along a (not a whole number: that's what incommensurate means) |
| Propagation | [0.42 0 0] 1k |
| Cell | a 6.932 · b 12.636 · c 6.179 Å · α 90° · β 90° · γ 90° |
| Transition | 17 K (−256 °C) |
| Measured at | 4 K |
| Magnetic ions | Mn |
| Largest moment component | 2.279 μB |
| Method | NSD and NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| K1_1 | K | 0.345 | 0.1478 | 0 | ||||
| K1_2 | K | 0.845 | 0.3522 | 0 | ||||
| Mn1_1 | Mn | 0 | 0 | 0.25 | ||||
| S1_1 | S | 0.1953 | 0.8965 | 0 | ||||
| S1_2 | S | 0.6953 | 0.6035 | 0 |
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.
A. Bhutani et al. PHYSICAL REVIEW MATERIALS (2019) · doi:10.1103/PhysRevMaterials.3.064404
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.64_K2MnS2.mcif from MAGNDATA · entry page
sha256 of this copy: 9a6f9e25561599a56475c44caeff22fcdc4ebdeabee14ed2c5281e11086889d3
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.64_K2MnS2.mcif.