Research/Sitter/MAGNDATA / 0.143_Cr2TeO6.mcif

Cr₂TeO₆

MAGNDATA entry 0.143 · 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.

Structure · 10 properties

Magnetic group	P n′ n m BNS 58.395
Point group	m′mm
Parent space group	P 4₂/m n m No. 136
Spins	collinear · net moment 0 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 4.546 · b 4.546 · c 9.014 Å · α 90° · β 90° · γ 90°
Measured at	4.2 K
Magnetic ions	Cr
Largest moment component	2.45 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 n′ n m →

Atom sites · 4 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Cr1	Cr	0	0	0.3345	2.45	0	0	2.45
Te1	Te	0	0	0
O1	O	0.301	0.301	0
O2	O	0.31	0.31	0.337

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. Kunnmann et al. J. Phys. Chem Sol. (1968) · doi:10.1016/0022-3697(68)90187-X

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.143_Cr2TeO6.mcif from MAGNDATA · entry page

sha256 of this copy: 5ff61a2d9a2544672c62eb8046e07aba5c3236e2d73d9e51bfd5581da5b01d6c
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.143_Cr2TeO6.mcif.