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Spin lattice of BaMnFeF7Spin lattice of BaMnFeF7

BaMnFeF7

MAGNDATA entry 0.577 · source
s-wave compensated ferrimagnet
Opposite moments cancel, but the two sublattices aren't related by any symmetry, so the bands split like a ferromagnet's (s-wave).
Spin group ¹2/¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 84.9 K (−188 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP 21′/c′ BNS 14.79
Parent space groupP 21/c No. 14
Spinscollinear · net moment 0.558 μB per cell
Propagation[0 0 0] 1k
Cella 5.5075 · b 10.9584 · c 9.1427 Å · α 90° · β 94.57° · γ 90°
Transition84.9 K (−188 °C)
Measured at2 K
Magnetic ionsFe, Mn
Largest moment component4.1 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 21′/c′ →
Atom sites · 10 sites · CSV
siteelementxyzmambmc|m| (μB)
Ba1Ba0.2280.16850.0425
Mn1Mn0.81030.06310.3803−0.580−4.094.0849
Fe1Fe0.69260.12050.76650.7204.14.1058
F1F0.4040.28230.2853
F2F0.49930.02990.2515
F3F0.14450.39960.0107
F4F0.98370.48350.2807
F5F0.09720.73780.2144
F6F0.34660.64690.9398
F7F0.71590.40530.4754

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

P. Lacorre et al. JOURNAL OF SOLID STATE CHEMISTRY (1992) · doi:10.1016/0022-4596(92)90185-X

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.577_BaMnFeF7.mcif from MAGNDATA · entry page

sha256 of this copy: 1fc94128a9c432dfab85cd2c49a518dae8d506789c0c900ad5c6951e2bf24de4
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.577_BaMnFeF7.mcif.