Research/Sitter/MAGNDATA / 1.226_CeCo2Ge4O12.mcif

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Spin lattice of CeCo2Ge4O12Spin lattice of CeCo2Ge4O12

CeCo2Ge4O12

MAGNDATA entry 1.226 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 4.5 K (−269 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPb n n a BNS 52.315
Parent space groupP 4/n b m No. 125
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 9.7369 · b 9.7369 · c 9.6252 Å · α 90° · β 90° · γ 90°
Transition4.5 K (−269 °C)
Measured at1.6 K
Magnetic ionsCo
Largest moment component2.29 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 Pb n n a →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Ce1Ce0.250.250.25
Co1Co000.252.291.1902.5807
Ge1_1Ge0.52440.250
Ge1_2Ge0.250.52440
O1O0.6310.3690.0903
O2_1O0.16190.06420.1285
O2_2O0.43580.16190.1285

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

D. Xu et al. Inorg. Chem. (2017) · doi:10.1021/acs.inorgchem.6b02905

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.226_CeCo2Ge4O12.mcif from MAGNDATA · entry page

sha256 of this copy: ce5125a814257cbac1d816f602b488dbb762b7a9176cde375093d4cbe0031643
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.226_CeCo2Ge4O12.mcif.