Research/Sitter/MAGNDATA / 0.1095_Y0.2La0.2Pr0.2Nd0.2Tb0.2MnO3.mcif

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Spin lattice of Y0.2La0.2Pr0.2Nd0.2Tb0.2Mn1O3Spin lattice of Y0.2La0.2Pr0.2Nd0.2Tb0.2Mn1O3

Y0.2La0.2Pr0.2Nd0.2Tb0.2Mn1O3

MAGNDATA entry 0.1095 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 67 K (−206 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP n′ m a′ BNS 62.448
Point groupm′m′m
Parent space groupP n m a No. 62
Spinsnoncoplanar · net moment 2 μB per cell
Propagation[0 0 0] 1k
Cella 5.742 · b 7.5359 · c 5.3891 Å · α 90° · β 90° · γ 90°
Transition67 K (−206 °C)
Measured at60 K
Magnetic ionsMn
Largest moment component0.5 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 · 8 sites · CSV
siteelementxyzmambmc|m| (μB)
Y1Y0.06730.250.9896
La1La0.06730.250.9896
Pr1Pr0.06730.250.9896
Nd1Nd0.06730.250.9896
Tb1Tb0.06730.250.9896
Mn1Mn000.50.3460.50.1460.6253
O1O0.47620.250.0867
O2O0.18350.54540.2111

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

Nathan D. Arndt et al. J. Mater. Chem. C (2024) · doi:10.1039/d4tc01411a

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1095_Y0.2La0.2Pr0.2Nd0.2Tb0.2MnO3.mcif from MAGNDATA · entry page

sha256 of this copy: deb4047cee6e7708197e3828e0e70c636f3f6879d00153e7b639e742317ffd31
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1095_Y0.2La0.2Pr0.2Nd0.2Tb0.2MnO3.mcif.