Research/Sitter/MAGNDATA / 1.854_CoTeMoO6.mcif

Co₁Te₁Mo₁O₆

MAGNDATA entry 1.854 · source

p-wave magnet

Coplanar spins, no net moment, and a translation that reverses every spin: spin splitting that is odd in momentum (p-wave).

ordered ≤ 24 K (−249 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	P_c 2₁ 2₁ 2₁ BNS 19.28
Point group	2221′
Parent space group	P 2₁ 2₁ 2 No. 18
Spins	coplanar · net moment 0 μ_B per cell
Propagation	[0 0 1/2] 1k
Cell	a 5.2406 · b 5.0543 · c 17.6312 Å · α 90° · β 90° · γ 90°
Transition	24 K (−249 °C)
Measured at	2 K
Magnetic ions	Co
Largest moment component	3.54 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_c 2₁ 2₁ 2₁ →

Atom sites · 6 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Co1	Co	0	0	0.262	0.59	3.54	0	3.5888
Te1	Te	0	0.5	0.127
Mo1	Mo	0	0.5	0.4045
O1	O	0.296	0.847	0.0365
O2	O	0.185	0.761	0.351
O3	O	0.179	0.72	0.196

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

Brady Wilson et al. Journal of Magnetism and Magnetic Materials (2025) · doi:10.1016/j.jmmm.2025.172963

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.854_CoTeMoO6.mcif from MAGNDATA · entry page

sha256 of this copy: f0cad4bfc6811f73c9268a14a7233aaeaa3fc25ed822ee568b42ff83c0feaf5b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.854_CoTeMoO6.mcif.

Co1Te1Mo1O6

Symmetry

Source

Original file

Co₁Te₁Mo₁O₆