Research/Sitter/MAGNDATA / 0.1150_ScFe2.mcif

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Spin lattice of Sc1Fe2Spin lattice of Sc1Fe2

Sc1Fe2

MAGNDATA entry 0.1150 · source
s-wave ferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Spin group ¹6/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 530 K (257 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC 2′/c′ BNS 15.89
Point group2′/m′
Parent space groupP 63/m m c No. 194
Spinscollinear · net moment 11.782 μB per cell
Propagation[0 0 0] 1k
Cella 4.9692 · b 4.9692 · c 8.1263 Å · α 90° · β 90° · γ 120°
Transition530 K (257 °C)
Measured at2 K
Magnetic ionsFe
Largest moment component1.282 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′/c′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Sc1Sc0.33330.66670.061
Fe1Fe0000.72501.2561.4502
Fe2_1Fe0.8320.6640.250.7401.2821.4802
Fe2_2Fe0.3360.1680.250.7401.2821.4802

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

S. El Bidaoui et al. Journal of Solid State Chemistry (2026) · doi:10.1016/j.jssc.2025.125754

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1150_ScFe2.mcif from MAGNDATA · entry page

sha256 of this copy: 4b486a5ee181c8fcc2afc8d9f53bd9983e308e58b40a94beec6d7c8a92d20413
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1150_ScFe2.mcif.