Research/Sitter/MAGNDATA / 0.397_Mn3Si2Te6.mcif

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Spin lattice of Mn3Si2Te6Spin lattice of Mn3Si2Te6

Mn3Si2Te6

MAGNDATA entry 0.397 · source
s-wave ferrimagnet
Opposite moments of different size leave a net magnetisation.
Spin group ¹3̄¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 78 K (−195 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC 2′/c′ BNS 15.89
Parent space groupP 3 1 c No. 163
Spinscollinear · net moment 8.4 μB per cell
Propagation[0 0 0] 1k
Cella 7.029 · b 7.029 · c 14.255 Å · α 90° · β 90° · γ 120°
Transition78 K (−195 °C)
Measured at4 K
Magnetic ionsMn
Largest moment component4.2 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 2′/c′ →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn0.33330.66670.00074.2004.2
Mn2Mn0.33330.66670.25−4.2004.2
Si1Si000.0815
Te1_1Te0.65870.00360.1279
Te1_2Te0.99640.65510.1279
Te1_3Te0.34490.34130.1279

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.F. May et al. PHYSICAL REVIEW B (2017) · doi:10.1103/PhysRevB.95.174440

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.397_Mn3Si2Te6.mcif from MAGNDATA · entry page

sha256 of this copy: adf1caca445e8cf826dd2586bb8ac06289e43882e9077724cac7f224717c0036
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.397_Mn3Si2Te6.mcif.