Research/Sitter/MAGNDATA / 1.633_YFe6Sn6.mcif

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Spin lattice of YFe6Sn6Spin lattice of YFe6Sn6

YFe6Sn6

MAGNDATA entry 1.633 · 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 ¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 558 K (285 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupPI n n n BNS 48.264
Point groupmmm1′
Parent space groupI m m m No. 71
Spinscollinear · net moment 0 μB per cell
Propagation[1 1 1] 1k
Cella 8.9021 · b 27.9891 · c 5.3932 Å · α 90° · β 90° · γ 90°
Transition558 K (285 °C)
Measured at293 K
Magnetic ionsFe
Largest moment component2.03 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 PI n n n →
Atom sites · 14 sites · CSV
siteelementxyzmambmc|m| (μB)
Y1Y000
Y2Y00.16740.5
Fe1Fe0.74580.50−2.03002.03
Fe2Fe0.250.250.252.03002.03
Fe3Fe0.75350.83450−2.03002.03
Fe4Fe0.24830.08370.24472.03002.03
Sn1Sn0.31500
Sn2Sn00.55540
Sn3Sn00.11280
Sn4Sn00.22450
Sn5Sn00.05640.5
Sn6Sn00.610.5
Sn7Sn00.72210.5
Sn8Sn0.83990.66810

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

J. M. Cadogan et al. JOURNAL OF APPLIED PHYSICS (2000) · doi:10.1063/1.372607

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.633_YFe6Sn6.mcif from MAGNDATA · entry page

sha256 of this copy: d361ade88376ced6e75390fc926e154039449a35209923819565cfcbd8c0c96d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.633_YFe6Sn6.mcif.