Research/Sitter/MAGNDATA / 0.57_ScFeO3.mcif

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Spin lattice of ScFeO3Spin lattice of ScFeO3

ScFeO3

MAGNDATA entry 0.57 · source
altermagnet
No net magnetisation, yet the electron bands are spin-split: the up and down spin sublattices are related only by a rotation or mirror, never by a shift or inversion.
Spin group ¹3̄²m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 360 K (87 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC c′ BNS 9.39
Point groupm′
Parent space groupR 3c No. 161
Spinscollinear · 3 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.2025 · b 5.2025 · c 14.0145 Å · α 90° · β 90° · γ 120°
Transition360 K (87 °C)
Measured at300 K
Magnetic ionsFe
Largest moment component2.72 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 c′ →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
O1_1O0.34230.97390.8176
O1_2O0.02610.36840.8176
O1_3O0.63160.65770.8176
Fe1Fe000.25792.72002.72
Fe2Fe000.0477−2.72002.72
Sc1Sc000.0477
Sc2Sc000.2579

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.-R. Li et al. J. Am. Chem. Soc. (2012) · doi:10.1021/ja208395z

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.57_ScFeO3.mcif from MAGNDATA · entry page

sha256 of this copy: 9459087e007046f6732d06d549d0314b88664553f2cb0aeb55740772fa00c99b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.57_ScFeO3.mcif.