Research/Sitter/MAGNDATA / 0.197_Co4Nb2O9.mcif

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Spin lattice of Co4Nb2O9Spin lattice of Co4Nb2O9

Co4Nb2O9

MAGNDATA entry 0.197 · 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 ≤ 28 K (−245 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2/c′ BNS 15.88
Parent space groupP 3 c 1 No. 165
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.1471 · b 5.1471 · c 14.0724 Å · α 90° · β 90° · γ 120°
Transition28 K (−245 °C)
Measured at5 K
Magnetic ionsCo
Largest moment component2.842 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 · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Nb1Nb000.3577
Co1Co0.33330.66670.0172.6771.31202.3185
Co2Co0.33330.66670.30782.8421.95302.5181
O1_1O0.290100.25
O1_2O00.29010.25
O2_1O0.34370.32050.0857
O2_2O0.67950.02320.0857
O2_3O0.97680.65630.0857

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. Deng et al. Phys. Rev. B (2018) · doi:10.1103/PhysRevB.97.085154

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.197_Co4Nb2O9.mcif from MAGNDATA · entry page

sha256 of this copy: 47399526d74647e0eb48e2ffb23164f00f5825242948c595b36a33ec1e926787
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.197_Co4Nb2O9.mcif.