Research/Sitter/MAGNDATA / 1.119_LaMn3V4O12.mcif

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Spin lattice of LaMn3V4O12Spin lattice of LaMn3V4O12

LaMn3V4O12

MAGNDATA entry 1.119 · source
noncollinear antiferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
ordered ≤ 44 K (−229 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupRI 3 BNS 148.20
Point group31′
Parent space groupI m 3 No. 204
Spinscoplanar · net moment 0 μB per cell
Propagation[1 0 0] 1k
Cella 7.4679 · b 7.4679 · c 7.4679 Å · α 90° · β 90° · γ 90°
Transition44 K (−229 °C)
Measured at2 K
Magnetic ionsMn
Largest moment component2.95 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 RI 3 →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn00.50.502.952.954.1719
V2V00.50.5
LaLa000
V1_1V0.250.250.25
V1_2V0.750.750.25
Mn2_1Mn0.250.250.25
Mn2_2Mn0.750.750.25
O_1O00.19330.2951
O_2O00.80670.2951

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

T. Saito et al. PHYSICAL REVIEW B (2014) · doi:10.1103/PhysRevB.90.214405

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.119_LaMn3V4O12.mcif from MAGNDATA · entry page

sha256 of this copy: c380b94d6db0ce481b729c6b59c0f09b382003635aeb39ede9a79417f6d0bd36
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.119_LaMn3V4O12.mcif.