Research/Sitter/MAGNDATA / 1.0.15_La0.33Sr0.67FeO3.mcif

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Spin lattice of La0.33Sr0.67FeO3Spin lattice of La0.33Sr0.67FeO3

La0.33Sr0.67FeO3

MAGNDATA entry 1.0.15 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 200 K (−73 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 32 2 1 BNS 154.41
Parent space groupR 3c No. 167
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[0 0 1] 1k
Cella 5.4822 · b 5.4822 · c 13.4052 Å · α 90° · β 90° · γ 120°
Transition200 K (−73 °C)
Measured at2 K
Magnetic ionsFe
Largest moment component3.67 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 32 2 1 →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
La1_1La000.25
La1_2La000.75
Sr1_1Sr000.25
Sr1_2Sr000.75
Fe1Fe0001.463.671.323.4619
O1_1O0.518100.25
O1_2O00.51810.25
O1_3O0.481900.75
O1_4O00.48190.75

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

F. Li et al. Phys. Rev. B (2018) · doi:10.1103/PhysRevB.97.174417

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.0.15_La0.33Sr0.67FeO3.mcif from MAGNDATA · entry page

sha256 of this copy: 4fc37578c7e88d44d752a24b641c3be7fb15a970391e6769458ec506ff7f7ad7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.0.15_La0.33Sr0.67FeO3.mcif.