Research/Sitter/MAGNDATA / 0.318_Tm2CoMnO6.mcif

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Spin lattice of Tm2CoMnO6Spin lattice of Tm2CoMnO6

Tm2CoMnO6

MAGNDATA entry 0.318 · source
noncoplanar 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
Spinsnoncoplanar · net moment 4.83 μB per cell
Propagation[0 0 0] 1k
Cella 5.18943 · b 5.54304 · c 7.41935 Å · α 90° · β 89.674° · γ 90°
Transition60 K (−213 °C)
Measured at2 K
Magnetic ionsCo, Mn, Tm
Largest moment component2.6 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)
Tm1Tm0.02080.07320.252−1.380.921.422.1783
Co1Co0.500.51.130−2.62.829
Mn1Mn0.5001.130−2.62.829
O1O0.30050.31730.0541
O2O0.32220.29340.4423
O3O0.61230.96260.2561

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

⬇ 0.318_Tm2CoMnO6.mcif from MAGNDATA · entry page

sha256 of this copy: 2c9f20732d150f069d1423cd41f6b06548c657fbb26454f7998d510d8daaf1ea
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.318_Tm2CoMnO6.mcif.