Research/Sitter/MAGNDATA / 1.649_Sr3ZnIrO6.mcif

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Spin lattice of Sr3ZnIrO6Spin lattice of Sr3ZnIrO6

Sr3ZnIrO6

MAGNDATA entry 1.649 · 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 2/c BNS 13.74
Point group2/m1′
Parent space groupR 3 c No. 167
Spinscoplanar · net moment 0 μB per cell
Propagation[0 1/2 1] 1k
Cella 9.66173 · b 19.32349 · c 11.23932 Å · α 90° · β 90° · γ 119.99995°
Transition17 K (−256 °C)
Measured at1.8 K
Magnetic ionsIr
Largest moment component0.67 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 PC 2/c →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Sr1Sr0.635900.75
Sr2Sr0.66670.84870.5833
Zn1Zn000.75
O1O0.17320.01030.1129
O2O−0.02060.07630.1129
O3O0.8474−0.08660.1129
Ir1Ir000−0.072−0.5790.670.8647

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.A. McClarty et al. J. Phys. Soc. Jpn. (2020) · doi:10.7566/JPSJ.89.064703

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.649_Sr3ZnIrO6.mcif from MAGNDATA · entry page

sha256 of this copy: 7d0bd11e82d992466b3ec72ba45199717c9c98ebd575867f6c90eb3af7b3a87f
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.649_Sr3ZnIrO6.mcif.