Research/Sitter/MAGNDATA / 2.53_Ba2Mn3Sb2O2.mcif

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Spin lattice of Ba2Mn3Sb2O2Spin lattice of Ba2Mn3Sb2O2

Ba2Mn3Sb2O2

MAGNDATA entry 2.53 · 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 ≤ 60 K (−213 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC m′ m a BNS 67.503
Parent space groupI 4/m m m No. 139
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] · [1/2 1/2 0] 2k
Cella 8.734 · b 8.734 · c 20.779 Å · α 90° · β 90° · γ 90°
Transition60 K (−213 °C)
Measured at6 K
Magnetic ionsMn
Largest moment component3.617 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 C m′ m a →
Atom sites · 7 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba000.417
Mn1_1Mn00.250.25003.6173.617
Mn1_2Mn00.750.25003.6173.617
Mn2Mn0002.52−2.5203.5638
Sb1Sb000.168
O1_1O00.250
O1_2O00.750

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

Q. Zhang et al. PHYSICAL REVIEW B (2019) · doi:10.1103/PhysRevB.99.184416

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.53_Ba2Mn3Sb2O2.mcif from MAGNDATA · entry page

sha256 of this copy: 9bb7706a7c808a70c87349fc8d250eb3bfd24470f0068a29992d7d7cad7c1ce8
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.53_Ba2Mn3Sb2O2.mcif.