Research/Sitter/MAGNDATA / 1.276_Na0.5Li0.5FeGe2O6.mcif

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Spin lattice of Na0.5Li0.5FeGe2O6Spin lattice of Na0.5Li0.5FeGe2O6

Na0.5Li0.5FeGe2O6

MAGNDATA entry 1.276 · 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 ≤ 18 K (−255 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPa 21/c BNS 14.80
Parent space groupP 21/c No. 14
Spinscollinear · net moment 0 μB per cell
Propagation[1/2 0 0] 1k
Cella 19.8314 · b 8.8161 · c 5.4471 Å · α 90° · β 109.509° · γ 90°
Transition18 K (−255 °C)
Measured at1.5 K
Magnetic ionsFe
Largest moment component4.3 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 Pa 21/c →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Li1Li0.130.0640.26
Na1Na0.130.0640.26
Fe1Fe0.120.65250.234.3004.3
Ge1Ge0.020.340.249
Ge2Ge0.2740.8440.241
O1O0.4270.3290.158
O2O0.0520.5190.285
O3O0.0550.2790.573
O4O0.1820.8360.116
O5O0.3110.020.34
O6O0.3090.710.494

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

T.V.Drokina et al. Journal of Magnetism and Magnetic Materials (2015) · doi:10.1016/j.jmmm.2015.03.01

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.276_Na0.5Li0.5FeGe2O6.mcif from MAGNDATA · entry page

sha256 of this copy: eeca3bfe3d3d6a3db56057ed4cbafd19a3b786315a5d93c1a825bb694d1b8676
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.276_Na0.5Li0.5FeGe2O6.mcif.