Research/Sitter/MAGNDATA / 0.1011_FeMn2O4.mcif

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Spin lattice of FeMn2O4Spin lattice of FeMn2O4

FeMn2O4

MAGNDATA entry 0.1011 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 65 K (−208 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupI m m′ a′ BNS 74.559
Point groupm′m′m
Parent space groupI 41/a m d No. 141
Spinscoplanar · net moment 8 μB per cell
Propagation[0 0 0] 1k
Cella 5.8945 · b 5.8945 · c 8.8855 Å · α 90° · β 90° · γ 90°
Transition65 K (−208 °C)
Measured at10 K
Magnetic ionsFe, Mn
Largest moment component4.65 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′ a′ →
Atom sites · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn00.750.1254.65004.65
Fe1Fe00.750.1254.65004.65
Fe2_1Fe000.5−2.89002.89
Fe2_2Fe0.250.750.75−2.760−1.313.0551
Mn2_1Mn000.5−2.89002.89
Mn2_2Mn0.250.750.75−2.760−1.313.0551
O1_1O00.4740.261
O1_2O0.7750.750.511

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

Q. Zhang et al. Chem. Mater. (2023) · doi:10.1021/acs.chemmater.2c03182

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1011_FeMn2O4.mcif from MAGNDATA · entry page

sha256 of this copy: 78e63183a54e84417368c96983629f8982dbb47ba42bbe23d3cce6365c9b8d27
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1011_FeMn2O4.mcif.