Research/Sitter/MAGNDATA / 0.554_Co2MnSi.mcif

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Spin lattice of Co2MnSiSpin lattice of Co2MnSi

Co2MnSi

MAGNDATA entry 0.554 · 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 ¹m¹3̄¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 1014 K (741 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupI 4/m m′ m′ BNS 139.537
Parent space groupF m 3 m No. 225
Spinscollinear · net moment 17.4 μB per cell
Propagation[0 0 0] 1k
Cella 5.6406 · b 5.6406 · c 5.6406 Å · α 90° · β 90° · γ 90°
Transition1014 K (741 °C)
Measured at298 K
Magnetic ionsCo, Mn
Largest moment component2.43 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 I 4/m m′ m′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Co1Co0.250.250.25000.960.96
Mn1Mn0.250.250.25
Mn2Mn000002.432.43
Co3Co000
Si1Si0.50.50.5

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

S.J. Ahmed et al. Journal of Alloys and Compounds (2019) · doi:10.1016/j.jallcom.2018.12.018

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.554_Co2MnSi.mcif from MAGNDATA · entry page

sha256 of this copy: 8998b8c775582e0d73f62be7a3401ec6775de87eaf39f33b5af14c8950c6362d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.554_Co2MnSi.mcif.