Research/Sitter/MAGNDATA / 0.1044_Cr5Te8.mcif

Cr₅Te₈

MAGNDATA entry 0.1044 · 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 ¹3̄¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.

ordered ≤ 235 K (−38 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	P 3 m′ 1 BNS 164.89
Point group	3m′
Parent space group	P 3 m 1 No. 164
Spins	collinear · net moment 4 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 3.8972 · b 3.8972 · c 5.9965 Å · α 90° · β 90° · γ 120°
Transition	235 K (−38 °C)
Measured at	3.3 K
Magnetic ions	Cr
Largest moment component	2 μ_B
Method	NPD

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 3 m′ 1 →

Atom sites · 3 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Te1	Te	0.3333	0.6667	0.7533
Cr1	Cr	0	0	0	0	0	2	2
Cr2	Cr	0	0	0.5	0	0	2	2

Moment components are along the crystal axes a, b, c (μ_B), as magCIF writes them. Symmetry generates the rest of the cell from these sites.

Source

W. Ren et al. ACTA METALLURGICA SINICA (2024) · doi:10.11900/0412.1961.2024.00008

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1044_Cr5Te8.mcif from MAGNDATA · entry page

sha256 of this copy: 3c02f497a84aa24a05b418f68a35c75c3dd50914204c71eac99a994c5e7d3f90
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1044_Cr5Te8.mcif.