Research/Sitter/MAGNDATA / 1.1.19_UPtGe.mcif
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| Magnetic group | Imm21′(α00)0s0s |
| Point group | mm21′ |
| Parent space group | I m m 2 No. 44 |
| Repeats every | 1.81 cells along a (not a whole number: that's what incommensurate means) |
| Propagation | [0.554 0 0] 1k |
| Cell | a 4.32 · b 7.17 · c 7.5 Å · α 90° · β 90° · γ 90° |
| Transition | 50 K (−223 °C) |
| Measured at | 4.2 K |
| Magnetic ions | U |
| Largest moment component | 1.8 μB |
| Method | NSD and polarized neutron diffraction |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| U1 | U | 0 | 0 | 0.625 | ||||
| U2 | U | 0 | 0.5 | 0.686 | ||||
| Pt1 | Pt | 0 | 0.7217 | 0.314 | ||||
| Ge1 | Ge | 0 | 0.206 | 0.984 |
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.
D. Mannix et al. PHYSICAL REVIEW B (2000) · doi:10.1103/PhysRevB.62.3801
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.19_UPtGe.mcif from MAGNDATA · entry page
sha256 of this copy: ebb92b250fca7a13641c50b8f9ee592de9f4bd3cb4524d04b2f8b708e1ff6649
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.19_UPtGe.mcif.