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Spin lattice of LaSr3Fe3O9Spin lattice of LaSr3Fe3O9

LaSr3Fe3O9

MAGNDATA entry 1.481 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered > 350 K (77 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPC b c m BNS 57.391
Parent space groupC m c m No. 63
Spinscollinear · net moment 0 μB per cell
Propagation[1 0 0] 1k
Cella 28.7559 · b 5.528 · c 5.4583 Å · α 90° · β 90° · γ 90°
Transition>350 K (77 °C)
Measured at8 K
Magnetic ionsFe
Largest moment component3.99 μB
MethodCombined NPD and XPD

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 PC b c m →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe0.39350.99830.2500−3.993.99
Fe2Fe0.750.43920.2500−3.583.58
La1La0.95180.0020.25
Sr1Sr0.95180.0020.25
La2La0.82850.98990.25
Sr2Sr0.82850.98990.25
O1O0.60870.750
O2O0.3860.750
O3O0.46280.97480.25
O4O0.30860.04390.25
O5O0.750.1080.359

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

Ø.S. Fjellvåg et al. Journal of Solid State Chemistry (2019) · doi:10.1016/j.jssc.2019.03.050

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.481_LaSr3Fe3O9.mcif from MAGNDATA · entry page

sha256 of this copy: 2ea235c5feb9996ddce00909f06335e6b6fb9f1db8cf66dd59d6366222f2b972
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.481_LaSr3Fe3O9.mcif.