Research/Sitter/MAGNDATA / 1.166_La2LiOsO6.mcif

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Spin lattice of La2LiOsO6Spin lattice of La2LiOsO6

La2LiOsO6

MAGNDATA entry 1.166 · 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 ¹1̄ × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 30 K (−243 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPS 1 BNS 2.7
Point group11′
Parent space groupP 21/n No. 14
Spinscollinear · net moment 0 μB per cell
Propagation[1/2 1/2 0] 1k
Cella 11.0886 · b 11.2624 · c 7.844 Å · α 90° · β 90.2° · γ 90°
Transition30 K (−243 °C)
Measured at3.5 K
Magnetic ionsOs
Largest moment component1.6 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 PS 1 →
Atom sites · 12 sites · CSV
siteelementxyzmambmc|m| (μB)
La1_1La0.24450.02350.248
La1_2La0.00550.27350.252
Li1_1Li0.250.250.5
Li1_2Li000
Os1_1Os0.250.250−0.21.60.81.8003
Os1_2Os000.5−0.21.60.81.8003
O1_1O0.1090.1450.04
O1_2O0.1410.3950.46
O2_1O0.290.24050.245
O2_2O0.960.49050.255
O3_1O0.15250.390.046
O3_2O0.09750.640.454

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

C.M. Thompson et al. PHYSICAL REVIEW B (2016) · doi:10.1103/PhysRevB.93.014431

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.166_La2LiOsO6.mcif from MAGNDATA · entry page

sha256 of this copy: a92b956b5e56fa2fd76c509528b6684f5c0b4cda05e000db3e4e0a69fa7a5cff
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.166_La2LiOsO6.mcif.