Research/Sitter/MAGNDATA / 0.100_YCr0.5Mn0.5O3.mcif

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Spin lattice of YCr0.5Mn0.5O3Spin lattice of YCr0.5Mn0.5O3

YCr0.5Mn0.5O3

MAGNDATA entry 0.100 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
Structure · 10 properties
Magnetic groupP n′ m a′ BNS 62.448
Point groupm′m′m
Parent space groupP n m a No. 62
Spinsnoncoplanar · net moment 1 μB per cell
Propagation[0 0 0] 1k
Cella 5.6278 · b 7.4767 · c 5.2507 Å · α 90° · β 90° · γ 90°
Measured at5 K
Magnetic ionsMn
Largest moment component1.83 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′ m a′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Y1Y0.57260.250.017
Cr1Cr000
Mn1Mn0000.630.251.831.9515
O1O0.9650.250.8931
O2O0.31210.0540.1965

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

H. James et al. Dalton Transactions (2014) · doi:10.1039/c4dt02503b

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.100_YCr0.5Mn0.5O3.mcif from MAGNDATA · entry page

sha256 of this copy: 493fac1a87bca3640158778fe8477dc73d3e385956bf6680f8c8e770b4347290
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.100_YCr0.5Mn0.5O3.mcif.