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Spin lattice of Pr3Ru4Al12Spin lattice of Pr3Ru4Al12

Pr3Ru4Al12

MAGNDATA entry 0.173 · 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 ≤ 39 K (−234 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupC m′ c′ m BNS 63.462
Parent space groupP 63/m m c No. 194
Spinscollinear · net moment 11.8 μB per cell
Propagation[0 0 0] 1k
Cella 8.858 · b 8.858 · c 9.624 Å · α 90° · β 90° · γ 120°
Transition39 K (−234 °C)
Measured at10 K
Magnetic ionsPr
Largest moment component3.1 μB
MethodSingle crystal ND

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 C m′ c′ m →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Pr1_1Pr0.19160.38330.25003.13.1
Pr1_2Pr0.61670.80840.25001.41.4
Ru1Ru000
Ru2_1Ru0.500
Ru2_2Ru00.50
Al1_1Al0.56180.12350.25
Al1_2Al0.87650.43820.25
Al2_1Al0.83770.67540.0756
Al2_2Al0.32460.16230.0756
Al3Al0.33330.66670.0078
Al4Al000.25

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

M.S. Henriques et al. PHYSICAL REVIEW B (2018) · doi:10.1103/PhysRevB.97.014431

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.173_Pr3Ru4Al12.mcif from MAGNDATA · entry page

sha256 of this copy: 0192bde2d00e75ea91f663a8ec5145c7253b677db83efe2147b2530d0320d29e
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.173_Pr3Ru4Al12.mcif.