Research/Sitter/MAGNDATA / 0.901_La0.3Y0.7Mn2Ge2.mcif
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| Magnetic group | I m′ m 2′ BNS 44.231 |
| Point group | m′m2′ |
| Parent space group | I 4/m m m No. 139 |
| Spins | coplanar · net moment 6.08 μB per cell |
| Propagation | [0 0 0] 1k |
| Cell | a 4.0604 · b 4.0604 · c 10.884 Å · α 90° · β 90° · γ 90° |
| Transition | 350 K (77 °C) |
| Measured at | 200 K |
| Magnetic ions | Mn |
| Largest moment component | 1.75 μB |
| Method | NPD |
| site | element | x | y | z | ma | mb | mc | |m| (μB) |
|---|---|---|---|---|---|---|---|---|
| Mn1 | Mn | 0 | 0.5 | 0.25 | 0 | −1.75 | 1.52 | 2.318 |
| La1 | La | 0 | 0 | 0 | ||||
| Y1 | Y | 0 | 0 | 0 | ||||
| Ge1 | Ge | 0 | 0 | 0.385 |
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.
G. Venturini et al. Journal of Alloys and Compounds (1995) · doi:10.1016/0925-8388(94)01496-5
Cite the original paper and MAGNDATA, not this mirror.
⬇ 0.901_La0.3Y0.7Mn2Ge2.mcif from MAGNDATA · entry page
sha256 of this copy: bea1d3f70a4270e457109797ee5e35f05de3123ed71be79b0b00b639071efb5a
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.901_La0.3Y0.7Mn2Ge2.mcif.