Research/Sitter/MAGNDATA / 0.1138_CoTeMoO6.mcif

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Spin lattice of Co1Te1Mo1O6Spin lattice of Co1Te1Mo1O6

Co1Te1Mo1O6

MAGNDATA entry 0.1138 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 24.8 K (−248 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 21 21′ 2′ BNS 18.19
Point group2′2′2
Parent space groupP 21 21 2 No. 18
Spinscoplanar · net moment 1.4 μB per cell
Propagation[0 0 0] 1k
Cella 5.2312 · b 5.055 · c 8.8079 Å · α 90° · β 90° · γ 90°
Transition24.8 K (−248 °C)
Measured at5 K
Magnetic ionsCo
Largest moment component3.6 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 P 21 21′ 2′ →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Co1Co000.47430.73.603.6674
Te1Te00.50.7466
Mo1Mo00.50.1927
O1O0.710.15320.9245
O2O0.81650.23820.2955
O3O0.82350.27910.6086

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

Chetan Dhital et al. PHYSICAL REVIEW MATERIALS (2025) · doi:10.1103/vqnq-rb68

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1138_CoTeMoO6.mcif from MAGNDATA · entry page

sha256 of this copy: 9993934be657d58d8b8274b606045b2c34bd55b8c464e39a5d6847a349d0e3b6
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1138_CoTeMoO6.mcif.