Research/Sitter/MAGNDATA / 1.391_Fe2MnBO5.mcif

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Spin lattice of Fe2MnBO5Spin lattice of Fe2MnBO5

Fe2MnBO5

MAGNDATA entry 1.391 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 90 K (−183 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPb n m a BNS 62.451
Parent space groupP b a m No. 55
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 9.5223 · b 12.4283 · c 6.1828 Å · α 90° · β 90° · γ 90°
Transition90 K (−183 °C)
Measured at70 K
Magnetic ionsFe
Largest moment component2.5 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 Pb n m a →
Atom sites · 14 sites · CSV
siteelementxyzmambmc|m| (μB)
Fe1Fe000
Fe2Fe00.50.2502.502.5
Fe3Fe0.00010.27530
Fe4Fe0.74110.38630.2501.801.8
Mn1Mn000
Mn2Mn00.50.25
Mn3Mn0.00010.27530
Mn4Mn0.74110.38630.25
B1B0.2710.3610.25
O1O0.8430.04320.25
O2O0.38520.07670
O3O0.62560.13860.25
O4O0.11350.1410
O5O0.8380.23610.25

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

F. Damay et al. PHYSICAL REVIEW B (2020) · doi:10.1103/PhysRevB.101.094418

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.391_Fe2MnBO5.mcif from MAGNDATA · entry page

sha256 of this copy: e53115b63b55e4ffd36a19f5d788b0a13850ede4a91e00a28e247a2feaa68cd7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.391_Fe2MnBO5.mcif.