Research/Sitter/MAGNDATA / 2.116_Na3Co2SbO6.mcif

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Spin lattice of Na3Co2Sb1O6Spin lattice of Na3Co2Sb1O6

Na3Co2Sb1O6

MAGNDATA entry 2.116 · 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 ≤ 5.5 K (−268 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupCa 2/m BNS 12.64
Point group2/m1′
Parent space groupC 2/m No. 12
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 1/2 0] · [1/2 -1/2 0] 2k
Cella 10.7414 · b 18.5782 · c 5.6533 Å · α 90° · β 108.566° · γ 90°
Transition5.5 K (−268 °C)
Measured at2 K
Magnetic ionsCo
Largest moment component1.27 μB
Methodsimulated 2k structure acording to the results reported in 10.1103/PhysRevB.109.L060410 by Gu et al.

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 2/m →
Atom sites · 12 sites · CSV
siteelementxyzmambmc|m| (μB)
Co1_1Co00.333300.69000.69
Co1_2Co0.250.5834001.2701.27
Sb2_1Sb000
Sb2_2Sb0.250.250
O1_1O0.13650.17060.7947
O1_2O0.38650.42060.7947
O2_1O0.375500.2044
O2_2O0.62560.250.2044
Na1_1Na00.250.5
Na1_2Na0.2500.5
Na2_1Na00.41380.5
Na2_2Na0.250.66380.5

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

V. O Garlea et al. Acta Cryst. B (2025) · doi:10.1107/S2052520624009831

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.116_Na3Co2SbO6.mcif from MAGNDATA · entry page

sha256 of this copy: ed74abfafebfdfc20c2cd4ab819779c49442f1bf99ea930951d9c1f9091b3a52
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.116_Na3Co2SbO6.mcif.