Research/Sitter/MAGNDATA / 0.1043_NdPt6Al3.mcif

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Spin lattice of Nd1Pt16Al3Spin lattice of Nd1Pt16Al3

Nd1Pt16Al3

MAGNDATA entry 0.1043 · source
noncollinear ferrimagnet
Opposite moments of different size leave a net magnetisation.
ordered ≤ 1.2 K (−272 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC 2/c1 BNS 15.85
Point group2/m1
Parent space groupR 3 c No. 167
Spinscoplanar · net moment 8.16 μB per cell
Propagation[0 0 0] 1k
Cella 7.5447 · b 7.5447 · c 39.2428 Å · α 90° · β 90° · γ 120°
Transition1.2 K (−272 °C)
Measured at0.05 K
Magnetic ionsNd
Largest moment component2.92 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 C 2/c1 →
Atom sites · 11 sites · CSV
siteelementxyzmambmc|m| (μB)
Nd1Nd000.08372.142.9202.6186
Pt1_1Pt0.212200.25
Pt1_2Pt00.21220.25
Pt2Pt000
Pt3Pt000.1626
Pt4_1Pt0.34430.01410.0389
Pt4_2Pt0.98590.33020.0389
Pt4_3Pt0.66980.65570.0389
Al1_1Al0.34850.00170.1917
Al1_2Al0.99830.34680.1917
Al1_3Al0.65320.65150.1917

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. Oishi et al. PHYSICAL REVIEW B (2024) · doi:10.1103/PhysRevB.110.144411

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1043_NdPt6Al3.mcif from MAGNDATA · entry page

sha256 of this copy: 0e6744a24d6ef7baec3269181e23e89bd6aae9f443d41b9d0e6be0476bbc05a5
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1043_NdPt6Al3.mcif.