Research/Sitter/MAGNDATA / 0.660_NdMn0.8Fe0.2O3.mcif

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Spin lattice of NdMn0.8Fe0.2O3Spin lattice of NdMn0.8Fe0.2O3

NdMn0.8Fe0.2O3

MAGNDATA entry 0.660 · source
noncoplanar ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 59 K (−214 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupP n′ m a′ BNS 62.448
Parent space groupP n m a No. 62
Spinsnoncoplanar · net moment 0.8 μB per cell
Propagation[0 0 0] 1k
Cella 5.781 · b 7.63 · c 5.439 Å · α 90° · β 90° · γ 90°
Transition59 K (−214 °C)
Measured at20 K
Magnetic ionsFe, Mn, Nd
Largest moment component2.91 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 n′ m a′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Nd1Nd0.0640.250.97300.700.7
Mn1Mn000.5−2.91−0.90.93.1762
Fe1Fe000.5
O1O0.4780.250.087
O2O0.3150.040.708

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

M. Mihalik et al. Physical Review B (2017) · doi:10.1103/PhysRevB.96.134430

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.660_NdMn0.8Fe0.2O3.mcif from MAGNDATA · entry page

sha256 of this copy: 27ff28bdc9f5e700712c6193f6962803f6e60208ffac83ad591bbd57b079bb4f
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.660_NdMn0.8Fe0.2O3.mcif.