Research/Sitter/MAGNDATA / 0.164_Y2MnCoO6.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Y2MnCoO6Spin lattice of Y2MnCoO6

Y2MnCoO6

MAGNDATA entry 0.164 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 80 K (−193 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 21′/c′ BNS 14.79
Point group2′/m′
Parent space groupP 21/c No. 14
Spinscoplanar · net moment 11.615 μB per cell
Propagation[0 0 0] 1k
Cella 5.21683 · b 5.56803 · c 7.44896 Å · α 90° · β 89.76° · γ 90°
Transition80 K (−193 °C)
Measured at2 K
Magnetic ionsCo, Mn
Largest moment component2.78 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)
Y1Y0.01930.07290.2512
Co1Co0.5000.850.33−2.782.9223
Mn1Mn00.500.850.33−2.782.9223
O1O0.29860.31540.0515
O2O0.31970.29240.4443
O3O0.60590.96610.2557

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 (2016) · doi:10.1103/PhysRevB.93.214401

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.164_Y2MnCoO6.mcif from MAGNDATA · entry page

sha256 of this copy: e3377c0a49dcd02c3dfa9da07d506bb2f153c3312b8633304b7fd7f8d2955e5c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.164_Y2MnCoO6.mcif.