Research/Sitter/MAGNDATA / 2.54_Sr2Cr3As2O2.mcif

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Spin lattice of Sr2Cr3As2O2Spin lattice of Sr2Cr3As2O2

Sr2Cr3As2O2

MAGNDATA entry 2.54 · 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 ≤ 291 K (18 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPC 21/c BNS 14.84
Parent space groupI 4/m m m No. 139
Spinscoplanar · net moment 0 μB per cell
Propagation[1 1 1] · [1/2 1/2 0] 2k
Cella 5.6553 · b 5.6553 · c 18.7151 Å · α 90° · β 90° · γ 90°
Transition291 K (18 °C)
Measured at4 K
Magnetic ionsCr
Largest moment component3.1 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 21/c →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Sr1Sr0.50.50.4113
As1As0.50.50.8308
Cr1Cr0.50.50003.13.1
Cr2_1Cr0.250.750.25−1.55−1.5502.192
Cr2_2Cr0.750.750.751.551.5502.192
O1_1O0.250.750
O1_2O0.750.750

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

J. Liu et al. PHYSICAL REVIEW B (2018) · doi:10.1103/PhysRevB.98.134416

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.54_Sr2Cr3As2O2.mcif from MAGNDATA · entry page

sha256 of this copy: 2fb42f0eb7f54a9db49284bb43a9e5109fb5070e43de1d06f3a7adc178dcc0bd
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.54_Sr2Cr3As2O2.mcif.