Research/Sitter/MAGNDATA / 1.0.16_La0.33Sr0.67FeO3.mcif

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

La0.33Sr0.67FeO3

MAGNDATA entry 1.0.16 · 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 ²2/²m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 200 K (−73 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2/c BNS 15.85
Parent space groupR 3c No. 167
Spinscollinear · 1 nodal planes · net moment 0 μB per cell
Propagation[0 0 1] 1k
Cella 9.4954 · b 5.4822 · c 13.4052 Å · α 90° · β 90° · γ 90°
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 C 2/c →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
La1_1La000.25
La1_2La0.16670.50.5833
Sr1_1Sr000.25
Sr1_2Sr0.16670.50.5833
Fe1_1Fe0003.26003.26
Fe1_2Fe0.16670.50.3333−3.67003.67
O1_1O0.25910.25910.25
O1_2O00.48190.25
O1_3O0.42570.75910.5833
O1_4O0.90760.75910.5833
O1_5O0.16670.98190.5833

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

⬇ 1.0.16_La0.33Sr0.67FeO3.mcif from MAGNDATA · entry page

sha256 of this copy: cf64ebe1cbca7677a366c5d8ec7d8be11aa8b8c0645592f63dd2f14f2bf215ef
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.0.16_La0.33Sr0.67FeO3.mcif.