Research/Sitter/MAGNDATA / 0.529_Co4Nb2O9.mcif

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Spin lattice of Co4Nb2O9Spin lattice of Co4Nb2O9

Co4Nb2O9

MAGNDATA entry 0.529 · 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 ≤ 27 K (−246 °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 5.18 · b 5.18 · c 14.163 Å · α 90° · β 90° · γ 120°
Transition27 K (−246 °C)
Measured at5 K
Magnetic ionsCo
Largest moment component3.201 μB
MethodNSD

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)
Co1Co0.33330.66670.0183.2012.1202.8204
Co2Co0.33330.66670.80683.2012.1202.8204
Nb1Nb000.3572
O1_1O0.29600.25
O1_2O00.2960.25
O2_1O0.3460.3030.0842
O2_2O0.6970.0430.0842
O2_3O0.9570.6540.0842

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

L. Ding et al. PHYSICAL REVIEW B (2020) · doi:10.1103/PhysRevB.102.174443

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.529_Co4Nb2O9.mcif from MAGNDATA · entry page

sha256 of this copy: ba489e42185200b460a01aec6e4ed1e5e2fe29f5b0f5c5c3dbc5e0f59ef82dd8
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.529_Co4Nb2O9.mcif.