Research/Sitter/MAGNDATA / 1.835_La2Co2O3Se2.mcif

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Spin lattice of La2Co2O3Se2Spin lattice of La2Co2O3Se2

La2Co2O3Se2

MAGNDATA entry 1.835 · 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 ≤ 217 K (−56 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupCA m c m BNS 63.468
Point groupmmm1′
Parent space groupI 4/m m m No. 139
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 1/2 0] 1k
Cella 5.73 · b 5.73 · c 18.3438 Å · α 90° · β 90° · γ 90°
Transition217 K (−56 °C)
Measured at10 K
Magnetic ionsCo
Largest moment component2.496 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 CA m c m →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
La1La0.750.750.6831
Co1Co000−2.496−2.49603.5299
O1O000.25
O2O0.750.750.5
Se1Se0.750.750.0952

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

Yayoi Fuwa et al. J. AM. CHEM. SOC. (2010) · doi:10.1021/ja109007g

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.835_La2Co2O3Se2.mcif from MAGNDATA · entry page

sha256 of this copy: 689fe767ec879c67d68a44ca941858710d959fd4a0558703678db14dac24cd33
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.835_La2Co2O3Se2.mcif.