Research/Sitter/MAGNDATA / 2.25_Sr2CoOsO6.mcif

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Spin lattice of Sr2CoOsO6Spin lattice of Sr2CoOsO6

Sr2CoOsO6

MAGNDATA entry 2.25 · 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 ≤ 70 K (−203 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPS 1 BNS 2.7
Parent space groupI 2/m No. 12
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 1/2 0] · [1/2 0 1/2] 2k
Cella 11.0122 · b 11.0158 · c 16.0516 Å · α 90° · β 90.62° · γ 90°
Transition70 K (−203 °C)
Measured at12 K
Magnetic ionsCo, Os
Largest moment component2.05 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 · 15 sites · CSV
siteelementxyzmambmc|m| (μB)
Sr1_1Sr0.2500.1251
Sr1_2Sr0.7500.8749
Os1Os0001.28−1.2801.8102
Co1_1Co000.252.050−2.052.9148
Co1_2Co0.250.2502.050−2.052.9148
O1_1O000.1212
O1_2O000.8788
O2_1O0.10240.14050
O2_2O0.89750.14050
O2_3O0.89750.85950
O2_4O0.10240.85950
O3_1O0.13890.39880
O3_2O0.86110.39880
O3_3O0.86110.60120
O3_4O0.13890.60120

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

R. Morrow et al. J. Amer. Chem. Soc. (2013) · doi:10.1021/ja407342w

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.25_Sr2CoOsO6.mcif from MAGNDATA · entry page

sha256 of this copy: d6a9d45669e1bc18dda9ab1c58a43b319e03f529e22a6a54f1ad78a073dffeef
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.25_Sr2CoOsO6.mcif.