Research/Sitter/MAGNDATA / 1.0.27_Li2MnTeO6.mcif

Li₂MnTeO₆

MAGNDATA entry 1.0.27 · source

noncollinear antiferromagnet

All moments add up to a net magnetisation: an ordinary magnet. Spin splitting is the same in every direction (s-wave).

ordered ≤ 8.5 K (−265 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 10 properties

Magnetic group	P 3 c 1 BNS 165.91
Parent space group	P 3 1 c No. 163
Spins	coplanar · net moment 0 μ_B per cell
Propagation	[1/3 1/3 0] 1k
Cell	a 15.0342 · b 15.0342 · c 9.4915 Å · α 90° · β 90° · γ 120°
Transition	8.5 K (−265 °C)
Measured at	1.6 K
Magnetic ions	Mn
Largest moment component	1.36 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 c 1 →

Atom sites · 7 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Mn1	Mn	0.2222	0.1111	0.25	0.68	1.36	0	1.1778
Li1	Li	0.1111	0.2222	0.0568
Te1_1	Te	0	0	0.25
Te1_2	Te	0	0.6667	0.25
O1_1	O	0.0152	0.2332	0.6364
O1_2	O	0.7668	0.9848	0.8636
O1_3	O	0.0152	0.8999	0.6364

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

E.A. Zvereva et al. Physical Review B (2020) · doi:10.1103/PhysRevB.102.094433

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.0.27_Li2MnTeO6.mcif from MAGNDATA · entry page

sha256 of this copy: 54a589659d7440dd413d39881ea0d14ad9ce3ac68054f6de845a08682b27982b
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.0.27_Li2MnTeO6.mcif.