Research/Sitter/MAGNDATA / 0.649_(Ho0.8Mn0.2)MnO3.mcif

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Spin lattice of (Ho0.8Mn0.2)MnO3Spin lattice of (Ho0.8Mn0.2)MnO3

(Ho0.8Mn0.2)MnO3

MAGNDATA entry 0.649 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 40 K (−233 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n m′ a′ BNS 62.447
Parent space groupP n m a No. 62
Spinscoplanar · net moment 25.84 μB per cell
Propagation[0 0 0] 1k
Cella 5.6329 · b 7.3908 · c 5.2461 Å · α 90° · β 90° · γ 90°
Transition40 K (−233 °C)
Measured at1.7 K
Magnetic ionsHo, Mn
Largest moment component5.22 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 n m′ a′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1Ho0.07830.250.9834−5.2202.685.8678
Mn1Mn0.07830.250.9834−3.57003.57
Mn2Mn000.52.33002.33
O1O0.46190.250.1059
O2O0.31830.05340.6983

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

A. Donni et al. Journal of Alloys and Compounds (2021) · doi:10.1016/j.jallcom.2020.158230

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.649_(Ho0.8Mn0.2)MnO3.mcif from MAGNDATA · entry page

sha256 of this copy: b00fd665b99ec53fc3cee604aaa793282777172a92bc934a436bb90fe2f8a911
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.649_(Ho0.8Mn0.2)MnO3.mcif.