Research/Sitter/MAGNDATA / 1.716_Sr2MnMoO6.mcif

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Spin lattice of Sr2Mn1Mo1O6Spin lattice of Sr2Mn1Mo1O6

Sr2Mn1Mo1O6

MAGNDATA entry 1.716 · 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 ≤ 12 K (−261 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPa 21/c BNS 14.80
Point group2/m1′
Parent space groupP 21/n No. 14
Spinscoplanar · net moment 0 μB per cell
Propagation[1/2 0 1/2] 1k
Cella 11.3342 · b 5.6537 · c 15.9938 Å · α 90° · β 89.93° · γ 90°
Transition12 K (−261 °C)
Measured at1.8 K
Magnetic ionsMn
Largest moment component3.5 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 Pa 21/c →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Sr1Sr0.49810.01760.1249
Mn1Mn0.25001.73.51.54.1709
Mo1Mo0.2500.25
O1O0.02730.49370.1182
O2O0.36820.28910.014
O3O0.10340.23280.4864

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

A. Munoz et al. J. Phys.: Condens. Matter (2002) · doi:10.1088/0953-8984/14/38/306

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.716_Sr2MnMoO6.mcif from MAGNDATA · entry page

sha256 of this copy: f787aa803ba362dcd8b0897e627c26e58823bce84067efcca5aab37d58aba69e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.716_Sr2MnMoO6.mcif.