Research/Sitter/MAGNDATA / 0.729_ErNi4B.mcif

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Spin lattice of ErNi4BSpin lattice of ErNi4B

ErNi4B

MAGNDATA entry 0.729 · 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 ≤ 10 K (−263 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 6/m m′ m′ BNS 191.240
Point group6/mm′m′
Parent space groupP 6/m m m No. 191
Spinscollinear · net moment 17.4 μB per cell
Propagation[0 0 0] 1k
Cella 4.9614 · b 4.9614 · c 6.936 Å · α 90° · β 90° · γ 120°
Transition10 K (−263 °C)
Measured at1.6 K
Magnetic ionsEr
Largest moment component8.7 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 P 6/m m′ m′ →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Er1Er000008.78.7
Er2Er000.5008.78.7
Ni1Ni0.33330.66670
Ni2Ni0.500.2899
B1B0.33330.66670.5

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

E. Alleno et al. J. Solid State Chem. (2013) · doi:10.1016/j.jssc.2013.03.003

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.729_ErNi4B.mcif from MAGNDATA · entry page

sha256 of this copy: 65bb2885618c434afbd8646a66436ecd430525756b083ba97e992340e5be92fe
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.729_ErNi4B.mcif.