Research/Sitter/MAGNDATA / 0.810_Fe2WO6.mcif

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Spin lattice of Fe2WO6Spin lattice of Fe2WO6

Fe2WO6

MAGNDATA entry 0.810 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 240 K (−33 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP b c′ n′ BNS 60.423
Point groupm′m′m
Parent space groupP b c n No. 60
Spinscoplanar · net moment 3.6 μB per cell
Propagation[0 0 0] 1k
Cella 4.576 · b 16.766 · c 4.967 Å · α 90° · β 90° · γ 90°
Transition240 K (−33 °C)
Magnetic ionsFe
Largest moment component2.66 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 b c′ n′ →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe00.05640.250.902.662.8081
Fe2Fe00.72420.25001.961.96
W1W00.38720.25
O1O0.240.04090.5958
O2O0.27340.12710.0692
O3O0.2760.20350.5817

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

H. Pinto et al. Acta Cryst. A (1977) · doi:10.1107/s0567739477001648

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.810_Fe2WO6.mcif from MAGNDATA · entry page

sha256 of this copy: 638dfdcc748586fe217aff946169ebb76fc1ea79f7fb23a4b3ed4cfef5f242a1
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.810_Fe2WO6.mcif.