Research/Sitter/MAGNDATA / 1.0.33_FeF3.mcif

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Spin lattice of FeF3Spin lattice of FeF3

FeF3

MAGNDATA entry 1.0.33 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 97 K (−176 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 63/m BNS 176.143
Parent space groupP 6/m m m No. 191
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 7.402 · b 7.402 · c 7.569 Å · α 90° · β 90° · γ 120°
Transition97 K (−176 °C)
Measured at2 K
Magnetic ionsFe
Largest moment component4.07 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 63/m →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe0.5004.07004.07
F1F0.4960.0290.25
F2F0.2111−0.21110

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. Solid State Communications (1986) · doi:10.1016/0038-1098(86)90836-7

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.0.33_FeF3.mcif from MAGNDATA · entry page

sha256 of this copy: 00b5742208374ff698118d90dad29c2281bb729c668f6803423d7935f7516a3d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.0.33_FeF3.mcif.