Research/Sitter/MAGNDATA / 0.958_Mn3Si2Te6.mcif

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Spin lattice of Mn3Si2Te6Spin lattice of Mn3Si2Te6

Mn3Si2Te6

MAGNDATA entry 0.958 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 78 K (−195 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC 2′/c′ BNS 15.89
Point group2′/m′
Parent space groupP 3 1 c No. 163
Spinsnoncoplanar · net moment 11.807 μB per cell
Propagation[0 0 0] 1k
Cella 7.0196 · b 12.1583 · c 14.1419 Å · α 90° · β 90° · γ 90°
Transition78 K (−195 °C)
Measured at5 K
Magnetic ionsMn
Largest moment component4.13 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)
Mn1Mn00.33330.9981−3.421.50.953.8534
Mn2Mn00.33330.754.130−0.734.194
Si1Si000.5819
Te1_1Te0.82470.17080.6283
Te1_2Te0.34380.00230.6283
Te1_3Te0.33150.3270.6283

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

F. Ye et al. PHYSICAL REVIEW B (2022) · doi:10.1103/PhysRevB.106.L180402

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.958_Mn3Si2Te6.mcif from MAGNDATA · entry page

sha256 of this copy: 3694ab00d9ef02e066ac14a09386914fec61dc24f7e51fb91c07bf9a6c1a1efa
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.958_Mn3Si2Te6.mcif.