Research/Sitter/MAGNDATA / 1.1.123_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 | 4.41 cells along c (not a whole number: that's what incommensurate means) |
| Propagation | [0 0 0.227] 1k |
| Cell | a 4.103 · b 4.103 · c 10.901 Å · α 90° · β 90° · γ 90° |
| Transition | 100 K (−173 °C) |
| Measured at | 2 K |
| Magnetic ions | Mn, Nd |
| Largest moment component | 2.35 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Nd1 | Nd | 0 | 0 | 0 | −2.35 | 0 | 0 | 2.35 |
| Mn1 | Mn | 0 | 0.5 | 0.25 | −1.52 | 0 | 0 | 1.52 |
| 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.
⬇ 1.1.123_NdMn2Ge2.mcif from MAGNDATA · entry page
sha256 of this copy: 3f44d39d10f919a101e96098056596dd1535bc3ce511701161821b52f81f089a
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.1.123_NdMn2Ge2.mcif.