Research/Sitter/MAGNDATA / 2.66_FeSn2.mcif

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Spin lattice of FeSn2Spin lattice of FeSn2

FeSn2

MAGNDATA entry 2.66 · 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 ≤ 93 K (−180 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC c′ c a BNS 68.513
Parent space groupI 4/m c m No. 140
Spinscoplanar · net moment 0 μB per cell
Propagation[1 1 1] · [0 0 0] 2k
Cella 6.537 · b 6.537 · c 5.316 Å · α 90° · β 90° · γ 90°
Transition93 K (−180 °C)
Measured at5 K
Magnetic ionsFe
Largest moment component1.46 μB
MethodNPD and Mossbauer spectrosc.

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′ c a →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe000.251.460.7401.6368
Sn1_1Sn0.16110.66110
Sn1_2Sn0.33890.16110

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

G Venturini et al. J. Phys. F: Met. Phys. (1985) · doi:10.1088/0305-4608/15/2/016

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.66_FeSn2.mcif from MAGNDATA · entry page

sha256 of this copy: 15ccb78fb76ce2b2eb79469b4158ea369bfb5598c65c1edceeb3be08b701bcaf
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.66_FeSn2.mcif.