Research/Sitter/MAGNDATA / 0.1058_PrBaMn2O6.mcif

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Spin lattice of Pr1Ba1Mn2O6Spin lattice of Pr1Ba1Mn2O6

Pr1Ba1Mn2O6

MAGNDATA entry 0.1058 · 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 ≤ 309 K (36 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 4/m m′ m′ BNS 123.345
Point group4/mm′m′
Parent space groupP 4/m m m No. 123
Spinscollinear · net moment 3.02 μB per cell
Propagation[0 0 0] 1k
Cella 3.889 · b 3.889 · c 7.7317 Å · α 90° · β 90° · γ 90°
Transition309 K (36 °C)
Measured at283 K
Magnetic ionsMn
Largest moment component1.51 μB
MethodNSD

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 4/m m′ m′ →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn0.50.50.2469001.511.51
Pr1Pr000
Ba1Ba000.5
O1O0.50.50
O2O00.50.2297
O3O0.50.50.5

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. Blasco et al. Low Temp. Phys. (2024) · doi:10.1063/10.0028621

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1058_PrBaMn2O6.mcif from MAGNDATA · entry page

sha256 of this copy: 45b86de2a53e5d8e3b4ced53ec57a09a3920446b9be196ee4c55982f30c7cdcf
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1058_PrBaMn2O6.mcif.