Research/Sitter/MAGNDATA / 1.323_CoGeO3.mcif

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Spin lattice of CoGeO3Spin lattice of CoGeO3

CoGeO3

MAGNDATA entry 1.323 · 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 ≤ 32.5 K (−241 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPC 21/c BNS 14.84
Parent space groupC 2/c No. 15
Spinscoplanar · net moment 0 μB per cell
Propagation[0 1 0] 1k
Cella 9.6587 · b 8.9878 · c 5.1701 Å · α 90° · β 101.24° · γ 90°
Transition32.5 K (−241 °C)
Measured at4 K
Magnetic ionsCo
Largest moment component4.15 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 PC 21/c →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Co1Co00.90670.25−0.9602.542.8851
Co2Co00.26860.252.2604.154.3213
Ge1Ge0.30110.09410.2144
O1O0.11820.09090.1357
O2O0.38240.24450.3841
O3O0.36060.06790.9091

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.J. Redhammer et al. Phys Chem Minerals (2010) · doi:10.1007/s00269-009-0335-x

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.323_CoGeO3.mcif from MAGNDATA · entry page

sha256 of this copy: 736c89017c45473d7c2d446c3b11c909aa24a29d19cc969fbec37a848e80ded2
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.323_CoGeO3.mcif.