Research/Sitter/MAGNDATA / 0.700_TbMn6Sn6.mcif

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Spin lattice of TbMn6Sn6Spin lattice of TbMn6Sn6

TbMn6Sn6

MAGNDATA entry 0.700 · source
s-wave ferrimagnet
Opposite moments of different size leave a net magnetisation.
Spin group ¹6/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered < 300 K (27 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 6/m m′ m′ BNS 191.240
Parent space groupP 6/m m m No. 191
Spinscollinear · net moment 5.77 μB per cell
Propagation[0 0 0] 1k
Cella 5.53 · b 5.53 · c 9.023 Å · α 90° · β 90° · γ 120°
Transition<300 K (27 °C)
Measured at2 K
Magnetic ionsMn, Tb
Largest moment component8.57 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 6/m m′ m′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Tb1Tb000.5008.578.57
Mn1Mn0.500.2500−2.392.39
Sn1Sn0.33330.66670
Sn2Sn0.33330.66670.5
Sn3Sn000.177

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

B. Chafik et al. Journal of the Less-Common Metals (1991) · doi:10.1016/0022-5088(91)90359-C

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.700_TbMn6Sn6.mcif from MAGNDATA · entry page

sha256 of this copy: 2aff62fa9e7f129936ed9cd621cdd24a7ad3949e886cd1e1b722d32fffbfd44b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.700_TbMn6Sn6.mcif.