Research/Sitter/MAGNDATA / 0.430_Yb3Pt4.mcif

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Spin lattice of Yb3Pt4Spin lattice of Yb3Pt4

Yb3Pt4

MAGNDATA entry 0.430 · source
noncoplanar magnet
Spins pointing in three dimensions, not confined to a plane.
ordered ≤ 2.4 K (−271 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupR 3′ BNS 148.19
Parent space groupR 3 No. 148
Spinsnoncoplanar · net moment 0 μB per cell
Propagation[0 0 0] 1k
Cella 12.8687 · b 12.8687 · c 5.616 Å · α 90° · β 90° · γ 120°
Transition2.4 K (−271 °C)
Measured at1.4 K
Magnetic ionsYb
Largest moment component0.76 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 R 3′ →
Atom sites · 4 sites · CSV
siteelementxyzmambmc|m| (μB)
Pt1Pt000
Pt2Pt000.5
Pt3Pt0.26930.21710.2786
Yb4Yb0.04210.21110.23350.760.680.360.808

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

Y. Janssen et al. PHYSICAL REVIEW B (2010) · doi:10.1103/PhysRevB.81.064401

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.430_Yb3Pt4.mcif from MAGNDATA · entry page

sha256 of this copy: c3ee3d3333a5c2684a4bfb124f6c020159e125a30b96043265c4432c30ecad23
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.430_Yb3Pt4.mcif.