Research/Sitter/MAGNDATA / 0.610_Pr0.95K0.05MnO3.mcif

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Spin lattice of Pr0.95K0.05MnO3Spin lattice of Pr0.95K0.05MnO3

Pr0.95K0.05MnO3

MAGNDATA entry 0.610 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 85 K (−188 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n′ m a′ BNS 62.448
Parent space groupP b n m No. 62
Spinscoplanar · net moment 4.2 μB per cell
Propagation[0 0 0] 1k
Cella 5.448 · b 5.676 · c 7.579 Å · α 90° · β 90° · γ 90°
Transition85 K (−188 °C)
Measured at4 K
Magnetic ionsMn, Pr
Largest moment component2.64 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)
Mn1Mn0.50002.641.052.8411
Pr1Pr0.4840.4370.75
K1K0.4840.4370.75
O1O0.5780.0120.75
O2O0.7160.3040.036

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

Z. Jirak! et al. JOURNAL OF SOLID STATE CHEMISTRY (1997) · doi:[email protected]

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.610_Pr0.95K0.05MnO3.mcif from MAGNDATA · entry page

sha256 of this copy: 015859705f0a9cdf4e9c3a631562661a54a214ea1d6697068f175568bdc765b8
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.610_Pr0.95K0.05MnO3.mcif.