Research/Sitter/MAGNDATA / 1.1.125_PrCoAl4.mcif
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| Magnetic group | Pmma1′(0,0,γ)ss0s |
| Point group | mmm1′ |
| Parent space group | P m m a No. 51 |
| Repeats every | 2.29 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.437] 1k |
| Cell | a 7.644 · b 4.0431 · c 6.8717 Å · α 90° · β 90° · γ 90° |
| Transition | 17 K (−256 °C) |
| Measured at | 1.5 K |
| Magnetic ions | Pr |
| Largest moment component | 2.13 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Pr1 | Pr | 0.25 | 0 | 0.386 | ||||
| Co1 | Co | 0.25 | 0 | 0.807 | ||||
| Al1 | Al | 0 | 0 | 0 | ||||
| Al2 | Al | 0.25 | 0.5 | 0.037 | ||||
| Al3 | Al | 0.069 | 0.5 | 0.696 |
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.
P. Schobinger-Papamantellos et al. Journal of Magnetism and Magnetic Materials (2001) · doi:10.1016/S0304-8853(01)00062-2
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.125_PrCoAl4.mcif from MAGNDATA · entry page
sha256 of this copy: 318bc2811ce49eca74f157c00b6ef0ef690a2927d78b304007e167a9b3265bcb
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.125_PrCoAl4.mcif.