Research/Sitter/MAGNDATA / 0.797_SmBaMn2O5.mcif

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Spin lattice of SmBaMn2O5Spin lattice of SmBaMn2O5

SmBaMn2O5

MAGNDATA entry 0.797 · source
s-wave ferrimagnet
Opposite moments of different size leave a net magnetisation.
Spin group ¹4/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 134 K (−139 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 4/n m′ m′ BNS 129.417
Point group4/mm′m′
Parent space groupP 4/n m m No. 129
Spinscollinear · net moment 1.82 μB per cell
Propagation[0 0 0] 1k
Cella 5.5449 · b 5.5449 · c 7.6165 Å · α 90° · β 90° · γ 90°
Transition134 K (−139 °C)
Measured at12 K
Magnetic ionsMn
Largest moment component4.06 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/n m′ m′ →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba0.750.250
Sm1Sm0.750.250.5
Mn1Mn0.250.250.2731003.153.15
Mn2Mn0.250.250.748200−4.064.06
O1O0.250.250.0062
O2O0.49050.49050.31

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. Materials Research Bulletin (2022) · doi:10.1016/j.materresbull.2022.111780

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.797_SmBaMn2O5.mcif from MAGNDATA · entry page

sha256 of this copy: c62f8235aa7e36f01e58a9661370271f6ab294636ccf3f8d24c7db900dbe1156
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.797_SmBaMn2O5.mcif.