Research/Sitter/MAGNDATA / 1.277_LiFeCr4O8.mcif

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Spin lattice of LiFeCr4O8Spin lattice of LiFeCr4O8

LiFeCr4O8

MAGNDATA entry 1.277 · source
s-wave ferrimagnet
Opposite moments of different size leave a net magnetisation.
Spin group ¹m¹3̄¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 94 K (−179 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupI 4 m′ 2′ BNS 119.319
Parent space groupF 4 3 m No. 216
Spinscollinear · net moment 5.68 μB per cell
Propagation[0 0 0] 1k
Cella 8.2778 · b 8.2778 · c 8.2778 Å · α 90° · β 90° · γ 90°
Transition94 K (−179 °C)
Measured at30 K
Magnetic ionsCr, Fe
Largest moment component2.54 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 I 4 m′ 2′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Li1Li000
Fe1Fe0.750.750.7500−2.542.54
Cr1Cr0.37260.37260.3726000.280.28
O1O0.13720.13720.1372
O2O0.61710.61710.6171

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

R. Saha et al. PHYSICAL REVIEW B (2017) · doi:10.1103/PhysRevB.96.214439

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.277_LiFeCr4O8.mcif from MAGNDATA · entry page

sha256 of this copy: cad23fe13b44db56f86fe0a92540d0828a159879f31cb7ea050271c2b397ab1c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.277_LiFeCr4O8.mcif.