Research/Sitter/MAGNDATA / 0.661_(Lu0.6Mn0.4)MnO3.mcif

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Spin lattice of (Lu0.6Mn0.4)MnO3Spin lattice of (Lu0.6Mn0.4)MnO3

(Lu0.6Mn0.4)MnO3

MAGNDATA entry 0.661 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 67 K (−206 °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 6.56 μB per cell
Propagation[0 0 0] 1k
Cella 5.4592 · b 7.365 · c 5.1783 Å · α 90° · β 90° · γ 90°
Transition67 K (−206 °C)
Measured at2.2 K
Magnetic ionsMn
Largest moment component4.87 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)
Mn1Mn000.53.23003.23
Mn2Mn0.0870.250.951−4.8701.425.0728
Lu1Lu0.08180.250.9701
O1O0.45680.250.1101
O2O0.3120.05490.6918

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

L. Zhang et al. Inorg. Chem. (2018) · doi:10.1021/acs.inorgchem.8b01470

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.661_(Lu0.6Mn0.4)MnO3.mcif from MAGNDATA · entry page

sha256 of this copy: 06f8ae2202769e8e4f92724614bf0a6da17b22debe521ca1ba8d79f2225e8f8a
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.661_(Lu0.6Mn0.4)MnO3.mcif.