Research/Sitter/MAGNDATA / 0.717_Pr0.5Sr0.4Ba0.1CoO3.mcif

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Spin lattice of Pr0.5Sr0.4Ba0.1CoO3Spin lattice of Pr0.5Sr0.4Ba0.1CoO3

Pr0.5Sr0.4Ba0.1CoO3

MAGNDATA entry 0.717 · source
s-wave ferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Spin group ¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 226 K (−47 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupI m′ m′ a BNS 74.558
Parent space groupI m m a No. 74
Spinscollinear · net moment 5.624 μB per cell
Propagation[0 0 0] 1k
Cella 5.3873 · b 7.609 · c 5.4246 Å · α 90° · β 90° · γ 90°
Transition226 K (−47 °C)
Measured at140 K
Magnetic ionsCo
Largest moment component1.406 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 I m′ m′ a →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Pr1Pr00.250.003
Sr1Sr00.250.003
Ba1Ba00.250.003
Co1Co000.5001.4061.406
O1O00.250.4631
O2O0.250.02060.75

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

J. Padilla-Pantoja et al. PHYSICAL REVIEW B (2021) · doi:10.1103/PhysRevB.104.054411

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.717_Pr0.5Sr0.4Ba0.1CoO3.mcif from MAGNDATA · entry page

sha256 of this copy: 7cb2686b9329b50a52883d28c0c7c9b7244f63ced8c39c5c715b8c9d23e2e734
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.717_Pr0.5Sr0.4Ba0.1CoO3.mcif.