Research/Sitter/MAGNDATA / 1.1.149_MnCr2O4.mcif
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| Magnetic group | F1(α,β,γ)0 |
| Point group | 11 |
| Parent space group | F d 3 m No. 227 |
| Repeats every | 1.52 cells along a (not a whole number: that's what incommensurate means) |
| Propagation | [0.65971 0.59989 0.19965] 1k |
| Cell | a 8.4271 · b 8.43062 · c 8.42597 Å · α 90° · β 90° · γ 90° |
| Transition | 18 K (−255 °C) |
| Measured at | 1.6 K |
| Magnetic ions | Cr, Mn |
| Largest moment component | 3.43 μB |
| Method | NPD at T = 1.6 K |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Mn1_1 | Mn | 0.125 | 0.125 | 0.125 | −2.2 | 2.2 | 0 | 3.1113 |
| Mn1_2 | Mn | 0.875 | 0.875 | 0.875 | −2.2 | 2.2 | 0 | 3.1113 |
| Cr1_1 | Cr | 0.5 | 0.5 | 0.5 | 0.79 | −0.79 | 0 | 1.1172 |
| Cr1_2 | Cr | 0.25 | 0.75 | 0 | 0.79 | −0.79 | 0 | 1.1172 |
| Cr1_3 | Cr | 0.75 | 0 | 0.25 | 0.73 | −0.73 | 0 | 1.0324 |
| Cr1_4 | Cr | 0 | 0.75 | 0.25 | 0.73 | −0.73 | 0 | 1.0324 |
| O1_1 | O | 0.7362 | 0.7362 | 0.7362 | ||||
| O1_2 | O | 0.7362 | 0.0138 | 0.0138 | ||||
| O1_3 | O | 0.0138 | 0.7362 | 0.0138 | ||||
| O1_4 | O | 0.0138 | 0.0138 | 0.7362 | ||||
| O1_5 | O | 0.2638 | 0.2638 | 0.2638 | ||||
| O1_6 | O | 0.2638 | −0.0138 | −0.0138 | ||||
| O1_7 | O | −0.0138 | 0.2638 | −0.0138 | ||||
| O1_8 | O | −0.0138 | −0.0138 | 0.2638 |
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. Pardo-Sainz et al. Physical Review B (2023) · doi:10.1103/PhysRevB.107.144401
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.149_MnCr2O4.mcif from MAGNDATA · entry page
sha256 of this copy: a7af75c66ea0cdc74f5cd3b3332322cbccf7377803789fc95380c8f1d1237f06
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.149_MnCr2O4.mcif.