Research/Sitter/MAGNDATA / 0.319_Tm2CoMnO6.mcif

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Spin lattice of Tm2CoMnO6Spin lattice of Tm2CoMnO6

Tm2CoMnO6

MAGNDATA entry 0.319 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 60 K (−213 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 21′/c′ BNS 14.79
Parent space groupP 21/c No. 14
Spinscoplanar · net moment 7.48 μB per cell
Propagation[0 0 0] 1k
Cella 5.18906 · b 5.54327 · c 7.41875 Å · α 90° · β 89.668° · γ 90°
Transition60 K (−213 °C)
Measured at25 K
Magnetic ionsCo, Mn, Tm
Largest moment component2.35 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 21′/c′ →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Tm1Tm0.01990.07310.2522−0.5800.530.7834
Co1Co0.500.51.020−2.352.5564
Mn1Mn0.5001.020−2.352.5564
O1O0.30150.31720.0538
O2O0.32340.29330.442
O3O0.61190.96110.2567

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

J. Blasco et al. PHYSICAL REVIEW B (2017) · doi:10.1103/PhysRevB.96.024409

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.319_Tm2CoMnO6.mcif from MAGNDATA · entry page

sha256 of this copy: 3c22a184980cccf4028899a491b28d6334acfc483ea61f0405bc0893d4b4b2aa
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.319_Tm2CoMnO6.mcif.