Research/Sitter/MAGNDATA / 1.819_(Ho0.54Lu0.46)2Fe2Si2C.mcif

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Spin lattice of Ho1.08Lu0.92Fe2Si2C1Spin lattice of Ho1.08Lu0.92Fe2Si2C1

Ho1.08Lu0.92Fe2Si2C1

MAGNDATA entry 1.819 · source
antiferromagnet
No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.
Spin group ¹2/¹m × ²1: 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 groupCc 2/m BNS 12.63
Point group2/m1′
Parent space groupC 2/m No. 12
Spinscollinear · net moment 0 μB per cell
Propagation[0 0 1/2] 1k
Cella 10.4707 · b 3.8837 · c 13.2638 Å · α 90° · β 129.076° · γ 90°
Transition10 K (−263 °C)
Measured at3 K
Magnetic ionsHo
Largest moment component9.1 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 Cc 2/m →
Atom sites · 5 sites · CSV
siteelementxyzmambmc|m| (μB)
Ho1Ho0.561600.147509.109.1
Lu1Lu0.561600.1475
Fe1Fe0.20400.049
Si1Si0.15800.351
C1C000

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. A. Susilo et al. J. Magn. Magn. Mat. (2024) · doi:10.1016/j.jmmm.2024.172631

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.819_(Ho0.54Lu0.46)2Fe2Si2C.mcif from MAGNDATA · entry page

sha256 of this copy: 99534ecb9316c5f6aa9a55ba38ab12593b481cdfb939d6fe78bfda858863a974
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.819_(Ho0.54Lu0.46)2Fe2Si2C.mcif.