Research/Sitter/MAGNDATA / 2.61_Fe3F8(H2O)2.mcif

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Spin lattice of Fe3F8(H2O)2Spin lattice of Fe3F8(H2O)2

Fe3F8(H2O)2

MAGNDATA entry 2.61 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 35 K (−238 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2′/m′ BNS 12.62
Parent space groupC 2/m No. 12
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[0 0 0] · [0 1 1/2] 2k
Cella 7.543 · b 7.4314 · c 14.773 Å · α 90° · β 117.26° · γ 90°
Transition35 K (−238 °C)
Measured at2 K
Magnetic ionsFe
Largest moment component4.2 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 2′/m′ →
Atom sites · 13 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1_1Fe0.250.250.251.654.030.434.301
Fe1_2Fe0.750.250.25−1.65−4.03−0.434.301
Fe2_1Fe00.504.203.233.9555
Fe2_2Fe0.500−4.20−3.233.9555
F1F00.29920.25
F2_1F0.178100.2197
F2_2F0.67810.50.2197
F3_1F0.13360.29620.1063
F3_2F0.63360.79620.1063
O1_1O0.24700.0278
O1_2O0.7470.50.0278
H1_1H0.2090.10020.054
H1_2H0.7090.60020.054

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

M. Leblanc et al. Journal of Magnetism and Magnetic Materials (1991) · doi:10.1016/0304-8853(91)90849-6

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.61_Fe3F8(H2O)2.mcif from MAGNDATA · entry page

sha256 of this copy: 55e73ce3f661259c81ba7f3d51ad34f0feedcf295b823fc9ea1cf2ce5fef8641
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.61_Fe3F8(H2O)2.mcif.