Research/Sitter/MAGNDATA / 0.962_LiCrGe2O6.mcif

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Spin lattice of Li1Cr1Ge2O6Spin lattice of Li1Cr1Ge2O6

Li1Cr1Ge2O6

MAGNDATA entry 0.962 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹2/¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 6 K (−267 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 21′/c BNS 14.77
Point group2′/m
Parent space groupP 21/c No. 14
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 9.7914 · b 8.7156 · c 5.335 Å · α 90° · β 108.92° · γ 90°
Transition6 K (−267 °C)
Measured at1 K
Magnetic ionsCr
Largest moment component2.18 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 · 10 sites · CSV
siteelementxyzmambmc|m| (μB)
Li1Li0.25880.48560.722
Cr1Cr0.25090.65830.2142.1801.12.0994
Ge1Ge0.0470.34460.2759
Ge2Ge0.55460.84210.2288
O1O0.85680.33410.1738
O2O0.11460.52670.2851
O3O0.11740.29160.61
O4O0.36440.83080.1045
O5O0.63170.00580.3891
O6O0.61360.68810.4535

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

G. J. Redhammer et al. Phys. Chem. Minerals (2015) · doi:10.1007/s00269-015-0738-9

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.962_LiCrGe2O6.mcif from MAGNDATA · entry page

sha256 of this copy: 4f63b0c2b9d195bd4ef9c74e006177b9b8a92a913faffcd6f798aa4a033c641e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.962_LiCrGe2O6.mcif.