Research/Sitter/MAGNDATA / 0.305_Pr0.5Sr0.5CoO3.mcif

⬇ Download .mcif  ·  Data (JSON)

Spin lattice of Pr0.5Sr0.5CoO3Spin lattice of Pr0.5Sr0.5CoO3

Pr0.5Sr0.5CoO3

MAGNDATA entry 0.305 · 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 ¹4/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 120 K (−153 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupF m′ m′ m BNS 69.524
Parent space groupI 4/m c m No. 140
Spinscollinear · net moment 7.467 μB per cell
Propagation[0 0 0] 1k
Cella 5.3585 · b 5.3585 · c 7.7093 Å · α 90° · β 90° · γ 90°
Transition120 K (−153 °C)
Measured at15 K
Magnetic ionsCo
Largest moment component1.32 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 F m′ m′ m →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Pr1Pr00.50.25
Sr1Sr00.50.25
Co1Co0001.321.3201.8668
O1O000.25
O2_1O0.28490.78490
O2_2O0.21510.28490

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.L. Garcia-Munoz et al. PHYSICAL REVIEW B (2016) · doi:10.1103/PhysRevB.94.014411

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.305_Pr0.5Sr0.5CoO3.mcif from MAGNDATA · entry page

sha256 of this copy: f95521507a45f8cfa94d87630f6aec46925f15c87ba3f179103d02f800c8e2b8
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.305_Pr0.5Sr0.5CoO3.mcif.