Research/Sitter/MAGNDATA / 0.998_MnFe3O5.mcif

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Spin lattice of Mn1Fe3O5Spin lattice of Mn1Fe3O5

Mn1Fe3O5

MAGNDATA entry 0.998 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
Structure · 10 properties
Magnetic groupC c BNS 9.37
Point groupm1
Parent space groupC m c m No. 63
Spinsnoncoplanar · net moment 2.4 μB per cell
Propagation[0 0 0] 1k
Cella 2.9017 · b 9.8928 · c 12.6083 Å · α 90° · β 90° · γ 90°
Measured at75 K
Magnetic ionsFe, Mn
Largest moment component3.2 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 C c →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1_1Fe00.73450.11311.61.53.23.8794
Fe1_2Fe00.73450.3869−1.61.5−3.23.8794
Fe2Fe000−1.7−1−2.43.1064
Mn2Mn000
Mn1Mn00.48120.250−2.61.73.1064
Fe3Fe00.48120.25
O1O00.81880.25
O2_1O00.34690.0473
O2_2O00.34690.4527
O3_1O00.09920.141
O3_2O00.09920.359

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

K. H. Hong et al. J. Mater. Chem. C (2018) · doi:10.1039/c8tc00053k

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.998_MnFe3O5.mcif from MAGNDATA · entry page

sha256 of this copy: 60650130d93cbe2176c4bfff08f3428bc0b1b91d399aa2ab9fc506d7dce54c85
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.998_MnFe3O5.mcif.