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Spin lattice of LiMn6Sn6Spin lattice of LiMn6Sn6

LiMn6Sn6

MAGNDATA entry 0.699 · source
s-wave ferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Spin group ¹6/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 380 K (107 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC m m′ m′ BNS 65.486
Parent space groupP 6/m m m No. 191
Spinscollinear · net moment 15.48 μB per cell
Propagation[0 0 0] 1k
Cella 5.491 · b 5.491 · c 9.012 Å · α 90° · β 90° · γ 120°
Transition380 K (107 °C)
Measured at2 K
Magnetic ionsMn
Largest moment component2.58 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 C m m′ m′ →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1_1Mn0.500.2512.58002.58
Mn1_2Mn00.50.2512.58002.58
Sn1Sn0.33330.66670
Sn2Sn0.33330.66670.5
Sn3Sn000.18
Li1Li000.5

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

T. Mazet et al. Eur. Phys. J. B (2006) · doi:10.1140/epjb/e2006-00207-9

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.699_LiMn6Sn6.mcif from MAGNDATA · entry page

sha256 of this copy: 25fa45bbbffa44d1037b5042b5e32038cc1d9b1e035994b52bc2b7cabc2c5e58
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.699_LiMn6Sn6.mcif.