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Spin lattice of Ba2CoO4Spin lattice of Ba2CoO4

Ba2CoO4

MAGNDATA entry 1.476 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 25 K (−248 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPa 21/c BNS 14.80
Parent space groupP 21/n No. 14
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 11.8383 · b 7.6283 · c 20.8457 Å · α 90° · β 91.27° · γ 90°
Transition25 K (−248 °C)
Measured at1.8 K
Magnetic ionsCo
Largest moment component2.97 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 Pa 21/c →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Co1Co0.37380.27560.03992.97−1.13−1.33.4582
Ba1Ba0.37740.85080.0411
Ba2Ba0.12120.49190.095
O1O0.3810.50790.0411
O2O0.25520.19920.0823
O3O0.00040.1790.0722
O4O0.35920.1860.4598

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

G. Ryu et al. Phys. Status Solidi RRL (2019) · doi:10.1002/pssr.201800537

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.476_Ba2CoO4.mcif from MAGNDATA · entry page

sha256 of this copy: 365115aa41dacb7351acc3cee79082cb308070469c73c3b21f09eb2cffe058ba
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.476_Ba2CoO4.mcif.