Research/Sitter/MAGNDATA / 0.1139_Gd2CoRuO6.mcif

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Spin lattice of Gd2Co1Ru1O6Spin lattice of Gd2Co1Ru1O6

Gd2Co1Ru1O6

MAGNDATA entry 0.1139 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 51 K (−222 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 21/c1 BNS 14.75
Point group2/m1
Parent space groupP 21/n No. 14
Spinscoplanar · net moment 1.6 μB per cell
Propagation[0 0 0] 1k
Cella 5.318 · b 5.75 · c 7.592 Å · α 90° · β 89.9° · γ 90°
Transition51 K (−222 °C)
Measured at6 K
Magnetic ionsCo, Ru
Largest moment component1.64 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/c1 →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Co1Co0.50000.3−1.611.6377
Gd1Gd0.190.0740.248
Ru1Ru0.500.500.5−1.641.7145
O1O0.180.820.05
O2O0.310.290.05
O3O0.90.460.25

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

PHYSICAL REVIEW MATERIALS (2025) · doi:10.1103/fh1z-bxqt

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1139_Gd2CoRuO6.mcif from MAGNDATA · entry page

sha256 of this copy: ea0b8a5ed6eee3dc54081dda97363161118b70690e2044e258b619605f726792
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1139_Gd2CoRuO6.mcif.