Research/Sitter/MAGNDATA / 0.1168_Fe2SiSe4.mcif

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Spin lattice of Fe2SiSe4Spin lattice of Fe2SiSe4

Fe2SiSe4

MAGNDATA entry 0.1168 · 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 ≤ 110 K (−163 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n m a1 BNS 62.441
Point groupm m m1
Parent space groupP n m a No. 62
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 13.02 · b 7.544 · c 6.119 Å · α 90° · β 90° · γ 90°
Transition110 K (−163 °C)
Measured at80 K
Magnetic ionsFe
Largest moment component4.04 μB
MethodNPD. Rietveld refinements were performed with the FULLPROF SUITE and representation analysis with SARAh.

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 n m a1 →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe0000.431.3801.4454
Fe2Fe0.22830.250.51160−4.0404.04
Si1Si0.40740.250.0734
Se1Se0.40820.250.7239
Se2Se0.57140.250.2399
Se3Se0.33320.0160.2481

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

Feihao Pan et al. Phys. Rev. B (2023) · doi:10.1103/PhysRevB.107.224423

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1168_Fe2SiSe4.mcif from MAGNDATA · entry page

sha256 of this copy: 02b596cc20749c0591f7e3fa140dcdc48b6c3a7f0149c96241911522ee7852b9
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1168_Fe2SiSe4.mcif.