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Spin lattice of MnFe4Si3Spin lattice of MnFe4Si3

MnFe4Si3

MAGNDATA entry 0.674 · 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 ≤ 260 K (−13 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 63/m c′ m′ BNS 193.260
Parent space groupP 63/m c m No. 193
Spinscollinear · net moment 35.6 μB per cell
Propagation[0 0 0] 1k
Cella 6.8043 · b 6.8043 · c 4.7254 Å · α 90° · β 90° · γ 120°
Transition260 K (−13 °C)
Measured at10 K
Magnetic ionsFe, Mn
Largest moment component2.1 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 63/m c′ m′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn0.33330.66670001.31.3
Fe1Fe0.33330.66670001.31.3
Mn2Mn0.242700.25002.12.1
Fe2Fe0.242700.25002.12.1
Si1Si0.600500.25

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

O. Gourdon et al. Journal of Solid State Chemistry (2014) · doi:10.1016/j.jssc.2014.05.001

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.674_MnFe4Si3.mcif from MAGNDATA · entry page

sha256 of this copy: daeb83bed9b4161d9a27a30ffde033274d6df1411c519ecab11cf07e5b688c50
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.674_MnFe4Si3.mcif.