Research/Sitter/MAGNDATA / 0.416_LaCrO3.mcif

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Spin lattice of LaCrO3Spin lattice of LaCrO3

LaCrO3

MAGNDATA entry 0.416 · 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 ≤ 380 K (107 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupR 3 c BNS 167.103
Parent space groupR 3 c No. 167
Spinscollinear · 3 nodal planes · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.4599 · b 5.4599 · c 13.1307 Å · α 90° · β 90° · γ 120°
Transition380 K (107 °C)
Measured at295 K
Magnetic ionsCr
Largest moment component1.67 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 R 3 c →
Atom sites · 3 sites · CSV
siteelementxyzmambmc|m| (μB)
La1La000.25
Cr1Cr000001.671.67
O1O0.556800.25

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

J.-S. Zhou et al. PHYSICAL REVIEW LETTERS (2011) · doi:10.1103/PhysRevLett.106.057201

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.416_LaCrO3.mcif from MAGNDATA · entry page

sha256 of this copy: 115eb55642866bd9bbe86d4afe2a195ba6520dc077d70641c2eb1795f58742e5
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.416_LaCrO3.mcif.