Research/Sitter/MAGNDATA / 0.719_Yb0.42Sc0.58FeO3.mcif

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Spin lattice of Yb0.42Sc0.58FeO3Spin lattice of Yb0.42Sc0.58FeO3

Yb0.42Sc0.58FeO3

MAGNDATA entry 0.719 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 165 K (−108 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 63 c′ m′ BNS 185.201
Parent space groupP 63 c m No. 185
Spinsnoncoplanar · net moment 4.698 μB per cell
Propagation[0 0 0] 1k
Cella 5.8605 · b 5.8605 · c 11.7061 Å · α 90° · β 90° · γ 120°
Transition165 K (−108 °C)
Measured at125 K
Magnetic ionsFe
Largest moment component2.511 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 c′ m′ →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
Yb1Yb000.2685
Sc1Sc000.2685
Yb2Yb0.33330.66670.2363
Sc2Sc0.33330.66670.2363
Fe1Fe0.3333002.51100.7832.6302
O1O0.330600.1704
O2O0.632300.338
O3O000.4763
O4O0.33330.66670.0124

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

Y. S. Tang et al. PHYSICAL REVIEW B (2021) · doi:10.1103/PhysRevB.103.174102

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.719_Yb0.42Sc0.58FeO3.mcif from MAGNDATA · entry page

sha256 of this copy: 52f22ebebdf38a9892d2bcdb00c72132d8089937f1eb714b11c077492bf0082c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.719_Yb0.42Sc0.58FeO3.mcif.