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Spin lattice of Pr6Fe13SnSpin lattice of Pr6Fe13Sn

Pr6Fe13Sn

MAGNDATA entry 1.450 · 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 ¹4/¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.
ordered ≤ 393 K (120 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 10 properties
Magnetic groupPI b c n BNS 60.432
Parent space groupI 4/m c m No. 140
Spinscollinear · net moment 0 μB per cell
Propagation[1 1 1] 1k
Cella 8.0925 · b 8.0925 · c 23.407 Å · α 90° · β 90° · γ 90°
Transition393 K (120 °C)
Measured at1.5 K
Magnetic ionsFe, Pr
Largest moment component2.91 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 b c n →
Atom sites · 9 sites · CSV
siteelementxyzmambmc|m| (μB)
Pr1Pr000.104402.9102.91
Pr2Pr0.16440.66440.186602.7302.73
Fe1Fe00.5002.302.3
Fe2_1Fe0.06550.2104002.5702.57
Fe2_2Fe0.78960.0655002.5702.57
Fe3_1Fe0.17850.67840.058802.4202.42
Fe3_2Fe0.32160.17850.058802.4202.42
Fe4Fe0.38650.88650.093702.5402.54
Sn1Sn000.25

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

P. Schobinger-Papamantellos et al. Journal of Magnetism and Magnetic Materials · doi:10.1016/S0304-8853(00)00351-6

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.450_Pr6Fe13Sn.mcif from MAGNDATA · entry page

sha256 of this copy: 3823e7bafc10f83da453d54c86ea57d30b51821c58f6540058d9dc6f356bbfe7
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.450_Pr6Fe13Sn.mcif.