Research/Sitter/MAGNDATA / 1.2_CuSe2O5.mcif

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Spin lattice of CuSe2O5Spin lattice of CuSe2O5

CuSe2O5

MAGNDATA entry 1.2 · 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 ≤ 17 K (−256 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPc 21/c BNS 14.84
Point group2/m1′
Parent space groupC 2/c No. 15
Spinscoplanar · net moment 0 μB per cell
Propagation[1 0 0] 1k
Cella 12.254 · b 4.858 · c 7.96 Å · α 90° · β 110.7° · γ 90°
Transition17 K (−256 °C)
Measured at6 K
Magnetic ionsCu
Largest moment component0.5 μB
MethodNSD

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 Pc 21/c →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Cu1Cu0000.130.500.5166
Se1Se0.1399−0.43530.3299
O1O0.12580.2251−0.0131
O2O0.1256−0.22370.1584
O3O0−0.61680.25

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

M. Herak et al. Phys. Rev. B (2013) · doi:10.1103/physrevb.87.104413

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.2_CuSe2O5.mcif from MAGNDATA · entry page

sha256 of this copy: e153603dcb1d021e4674bd492392429b5bf3710adc172832169169e6b9b21209
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.2_CuSe2O5.mcif.