Research/Sitter/MAGNDATA / 0.440_SrCuTe2O6.mcif

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Spin lattice of SrCuTe2O6Spin lattice of SrCuTe2O6

SrCuTe2O6

MAGNDATA entry 0.440 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 5.3 K (−268 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 41 3 2 BNS 213.63
Parent space groupP 41 3 2 No. 213
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 12.4321 · b 12.4321 · c 12.4321 Å · α 90° · β 90° · γ 90°
Transition5.25 K (−268 °C)
Measured at1.5 K
Magnetic ionsCu
Largest moment component0.37 μB
MethodNPD and NSD

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 41 3 2 →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Te1Te0.33790.91920.0589
Sr1Sr0.05360.05360.0536
Sr2Sr0.8750.8750.875
Cu1Cu0.4760.8750.2740.370−0.370.5233
O1O0.67020.12710.1795
O2O0.43910.01630.2271
O3O0.2220.97660.1297

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

P. Saeaun et al. PHYSICAL REVIEW B (2020) · doi:10.1103/PhysRevB.102.134407

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.440_SrCuTe2O6.mcif from MAGNDATA · entry page

sha256 of this copy: 084e3ae4a53eafd80375b0ec61355aefb57aef0e5b8238978fd29d6078bd0b93
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.440_SrCuTe2O6.mcif.