Research/Sitter/MAGNDATA / 1.1.122_NdMn2Ge2.mcif
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| Magnetic group | Im2′m′(0,0,γ)s00 |
| Point group | m′m2′ |
| Parent space group | I 4/m m m No. 139 |
| Repeats every | 5.46 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.183] 1k |
| Cell | a 4.109 · b 4.109 · c 10.924 Å · α 90° · β 90° · γ 90° |
| Transition | 250 K (−23 °C) |
| Measured at | 150 K |
| Magnetic ions | Mn, Nd |
| Largest moment component | 2.27 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Nd1 | Nd | 0 | 0 | 0 | ||||
| Mn1 | Mn | 0 | 0.5 | 0.25 | −1.48 | 0 | 0 | 1.48 |
| Ge1 | Ge | 0 | 0 | 0.386 |
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.
R. Welter et al. Journal of AlAys and Compounds (1995) · doi:10.1016/0925-8388(94)01378-0
Cite the original paper and MAGNDATA, not this mirror.
⬇ 1.1.122_NdMn2Ge2.mcif from MAGNDATA · entry page
sha256 of this copy: 07a2091d2020a94f07eb720b436ce39fbf9d1b2997d90053dc352d383509e0f7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.122_NdMn2Ge2.mcif.