Research/Sitter/MAGNDATA / 0.977_NdPdIn.mcif

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Spin lattice of Nd1Pd1In1Spin lattice of Nd1Pd1In1

Nd1Pd1In1

MAGNDATA entry 0.977 · source
s-wave ferromagnet
All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).
Spin group ¹6/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 30 K (−243 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupC m′ BNS 8.34
Point groupm′
Parent space groupP 6 2 m No. 189
Spinscollinear · net moment 4.494 μB per cell
Propagation[0 0 0] 1k
Cella 7.6743 · b 7.6743 · c 3.994 Å · α 90° · β 90° · γ 120°
Transition30 K (−243 °C)
Measured at15 K
Magnetic ionsNd
Largest moment component1.15 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 m′ →
Atom sites · 6 sites · CSV
siteelementxyzmambmc|m| (μB)
Nd1_1Nd0.5840001.150.961.498
Nd1_2Nd00.584001.150.961.498
Pd1Pd000
Pd2Pd0.33330.66670.5
In1_1In0.248200.5
In1_2In00.24820.5

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

L. Gondek et al. Journal of Magnetism and Magnetic Materials (2005) · doi:10.1016/j.jmmm.2004.08.002

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.977_NdPdIn.mcif from MAGNDATA · entry page

sha256 of this copy: f9b9d6a970adcdfdeca7d70405fa15f5075cf1706efecc332ca77d2228082bbb
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.977_NdPdIn.mcif.