Research/Sitter/MAGNDATA / 0.901_La0.3Y0.7Mn2Ge2.mcif

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Spin lattice of La0.3Y0.7Mn2Ge2Spin lattice of La0.3Y0.7Mn2Ge2

La0.3Y0.7Mn2Ge2

MAGNDATA entry 0.901 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 350 K (77 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupI m′ m 2′ BNS 44.231
Point groupm′m2′
Parent space groupI 4/m m m No. 139
Spinscoplanar · net moment 6.08 μB per cell
Propagation[0 0 0] 1k
Cella 4.0604 · b 4.0604 · c 10.884 Å · α 90° · β 90° · γ 90°
Transition350 K (77 °C)
Measured at200 K
Magnetic ionsMn
Largest moment component1.75 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 m′ m 2′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Mn1Mn00.50.250−1.751.522.318
La1La000
Y1Y000
Ge1Ge000.385

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

G. Venturini et al. Journal of Alloys and Compounds (1995) · doi:10.1016/0925-8388(94)01496-5

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.901_La0.3Y0.7Mn2Ge2.mcif from MAGNDATA · entry page

sha256 of this copy: bea1d3f70a4270e457109797ee5e35f05de3123ed71be79b0b00b639071efb5a
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.901_La0.3Y0.7Mn2Ge2.mcif.