Research/Sitter/MAGNDATA / 0.736_LaBaMn2O6.mcif

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Spin lattice of LaBaMn2O6Spin lattice of LaBaMn2O6

LaBaMn2O6

MAGNDATA entry 0.736 · 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 ¹m¹3̄¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 270 K (−3 °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 m 3 m No. 221
Spinscollinear · net moment 3.5 μB per cell
Propagation[0 0 0] 1k
Cella 3.8978 · b 3.8978 · c 3.8978 Å · α 90° · β 90° · γ 90°
Transition270 K (−3 °C)
Measured at1.7 K
Magnetic ionsMn
Largest moment component3.5 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 P 4/m m′ m′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
La1La000
Ba1Ba000
Mn1Mn0.50.50.5003.53.5
O1_1O0.50.50
O1_2O00.50.5

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

F. Millange et al. Chem. Mater. (1998) · doi:10.1021/cm980130v

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.736_LaBaMn2O6.mcif from MAGNDATA · entry page

sha256 of this copy: eae4154416e2aea6f109cdadb0b7b7228e9f1a376964858e6fde7aca8d5bafbf
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.736_LaBaMn2O6.mcif.