Research/Sitter/MAGNDATA / 2.58_La0.73Tb0.27Mn2Si2.mcif

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Spin lattice of La0.73Tb0.27Mn2Si2Spin lattice of La0.73Tb0.27Mn2Si2

La0.73Tb0.27Mn2Si2

MAGNDATA entry 2.58 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Structure · 9 properties
Magnetic groupP n n m′ BNS 58.396
Parent space groupI 4/m m m No. 139
Spinscoplanar · net moment 0 μB per cell
Propagation[1 1 1] · [0 0 0] 2k
Cella 3.931 · b 3.931 · c 10.456 Å · α 90° · β 90° · γ 90°
Measured at293 K
Magnetic ionsMn, Tb
Largest moment component1.02 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 n n m′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
La1La000
Tb1Tb000
Mn1Mn00.50.250.9501.021.3939
Si1Si000.375

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

E. Gerasimov et al. Journal of Alloys and Compounds (2018) · doi:10.1016/j.jallcom.2017.10.050

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 2.58_La0.73Tb0.27Mn2Si2.mcif from MAGNDATA · entry page

sha256 of this copy: c3a15cd2fdfcb4d38f46f454bca8a6812dc5c60abd3eae1836cb5509d955baec
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 2.58_La0.73Tb0.27Mn2Si2.mcif.