Research/Sitter/MAGNDATA / 1.706_Ba2MnTeO6.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Ba2Mn1Te1O6Spin lattice of Ba2Mn1Te1O6

Ba2Mn1Te1O6

MAGNDATA entry 1.706 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹4/¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 20 K (−253 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupCA m c a BNS 64.480
Point groupmmm1′
Parent space groupF m 3 m No. 225
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 1] 1k
Cella 8.2066 · b 8.2066 · c 8.2066 Å · α 90° · β 90° · γ 90°
Transition20 K (−253 °C)
Measured at2.1 K
Magnetic ionsMn
Largest moment component4.34 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 CA m c a →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba0.250.250.25
Mn1Mn0004.34004.34
Te1Te0.50.50.5
O1_1O0.264600
O1_2O00.26460
O1_3O000.2646

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

O. H. J. Mustonen et al. Chem. Mater. (2020) · doi:10.1021/acs.chemmater.0c02971

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.706_Ba2MnTeO6.mcif from MAGNDATA · entry page

sha256 of this copy: 57fa21c7cfd1cf2d6863e85b3c7d0b42b8599e3e36e5a939531899e05e455e69
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.706_Ba2MnTeO6.mcif.