Research/Sitter/MAGNDATA / 0.1131_Cr7Te8.mcif

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Spin lattice of Cr7Te8Spin lattice of Cr7Te8

Cr7Te8

MAGNDATA entry 0.1131 · 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 ≤ 350 K (77 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.
Structure · 11 properties
Magnetic groupP 63/m m′ c′ BNS 194.270
Point group6/mm′m′
Parent space groupP 63/m m c No. 194
Spinscollinear · net moment 2.92 μB per cell
Propagation[0 0 0] 1k
Cella 4.0034 · b 4.0034 · c 6.2405 Å · α 90° · β 90° · γ 120°
Transition350 K (77 °C)
Measured at298 K
Magnetic ionsCr
Largest moment component1.46 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 63/m m′ c′ →
Atom sites · 2 sites · CSV
siteelementxyzmambmc|m| (μB)
Cr1Cr000001.461.46
Te1Te0.33330.66670.25

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

K. Guratinder et al. PHYSICAL REVIEW B (2026) · doi:10.1103/nfhl-8fkn

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1131_Cr7Te8.mcif from MAGNDATA · entry page

sha256 of this copy: 2748d0645bcd282a5d9dda188ca7c57a153bcc0cba757af9d661f0ad1aa76883
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1131_Cr7Te8.mcif.