Research/Sitter/MAGNDATA / 0.520_TbCoO3.mcif

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Spin lattice of TbCoO3Spin lattice of TbCoO3

TbCoO3

MAGNDATA entry 0.520 · 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 ≤ 3.3 K (−270 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n m′ a BNS 62.444
Parent space groupP b n m No. 62
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 5.2034 · b 5.389 · c 7.405 Å · α 90° · β 90° · γ 90°
Transition3.3 K (−270 °C)
Measured at0.25 K
Magnetic ionsTb
Largest moment component6.5 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 P n m′ a →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb−0.01240.06330.256.5−5.108.262
Co1Co0.500
O1O0.09240.47790.25
O2O0.69920.2970.0446

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

K. Knizek et al. Solid State Sciences (2014) · doi:10.1016/j.solidstatesciences.2013.12.001

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.520_TbCoO3.mcif from MAGNDATA · entry page

sha256 of this copy: b6cb9bbf3c69b2d728b75d16b47ab88401ab822dc90492d7e30015a8af4a1939
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.520_TbCoO3.mcif.