Research/Sitter/MAGNDATA / 2.83_ErMn2Ge2.mcif

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Spin lattice of ErMn2Ge2Spin lattice of ErMn2Ge2

ErMn2Ge2

MAGNDATA entry 2.83 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 8 K (−265 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP m′ m′ n BNS 59.409
Point groupm′m′m
Parent space groupI 4/m m m No. 139
Spinscoplanar · net moment 15.4 μB per cell
Propagation[1 1 1] · [0 0 0] 2k
Cella 3.881 · b 3.881 · c 10.627 Å · α 90° · β 90° · γ 90°
Transition8 K (−265 °C)
Measured at4.2 K
Magnetic ionsEr, Mn
Largest moment component7.7 μB
MethodNPD

Symmetry

Stereogram of the magnetic point group: each operation applied to one direction. Filled = upper hemisphere, ring = lower; red operations include time reversal. Lines are mirrors; polygons are 2/3/4/6-fold axes; the centre ring is inversion.

Every structure in P m′ m′ n →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Er1Er0007.7007.7
Mn1Mn00.50.25002.32.3
Ge1Ge000.3885

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.

Source

J. Leciejewicz et al. Journal of Magnetism and Magnetic Materials (1984) · doi:10.1016/0304-8853(84)90317-2

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.83_ErMn2Ge2.mcif from MAGNDATA · entry page

sha256 of this copy: e6d194bc7ca352f1226a013c19b4601358b0eb40fa23511ae0415573e6b77abd
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.83_ErMn2Ge2.mcif.