Research/Sitter/MAGNDATA / 0.657_PrMn2Ge2.mcif

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Spin lattice of PrMn2Ge2Spin lattice of PrMn2Ge2

PrMn2Ge2

MAGNDATA entry 0.657 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 330 K (57 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupI m′ m 2′ BNS 44.231
Parent space groupI 4/m m m No. 139
Spinscoplanar · net moment 4.2 μB per cell
Propagation[0 0 0] 1k
Cella 4.123 · b 4.123 · c 10.925 Å · α 90° · β 90° · γ 90°
Transition330 K (57 °C)
Measured at295 K
Magnetic ionsMn, Pr
Largest moment component2.19 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 I m′ m 2′ →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Pr1Pr000
Mn1Mn00.50.25−2.1901.052.4287
Ge1Ge000.381

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

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.

Original file

⬇ 0.657_PrMn2Ge2.mcif from MAGNDATA · entry page

sha256 of this copy: ca7543aff303d818f217c992c08793e78d206785b122711fea25987e72cf740c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.657_PrMn2Ge2.mcif.