Research/Sitter/MAGNDATA / 0.818_MnTa2O6.mcif

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Spin lattice of MnTa2O6Spin lattice of MnTa2O6

MnTa2O6

MAGNDATA entry 0.818 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Structure · 10 properties
Magnetic groupP b′ c n BNS 60.419
Point groupm′mm
Parent space groupP b c n No. 60
Spinscoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 14.4219 · b 5.7513 · c 5.0816 Å · α 90° · β 90° · γ 90°
Measured at2 K
Magnetic ionsMn
Largest moment component3.25 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 P b′ c n →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn00.17350.253.2502.734.2445
Ta1Ta0.16230.32930.7519
O1O0.09940.40450.4306
O2O0.08290.10860.8947
O3O0.25880.12920.5838

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

S. Klein et al. Acta Cryst. A (1976) · doi:10.1107/S0567739476001253

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.818_MnTa2O6.mcif from MAGNDATA · entry page

sha256 of this copy: aec2312c8f219a87800f7c5e3c991644893ff28089d6dcdc80e54f04745f0a7c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.818_MnTa2O6.mcif.