Research/Sitter/MAGNDATA / 0.291_Tl2NiMnO6.mcif

Tl₂NiMnO₆

MAGNDATA entry 0.291 · 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 ¹2/¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.

ordered ≤ 80 K (−193 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 10 properties

Magnetic group	P 2₁/c BNS 14.75
Parent space group	P 2₁/c No. 14
Spins	collinear · net moment 5 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 5.2709 · b 5.3875 · c 7.6702 Å · α 90° · β 90.01° · γ 90°
Transition	80 K (−193 °C)
Measured at	1.5 K
Magnetic ions	Mn, Ni
Largest moment component	1.51 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 2₁/c →

Atom sites · 8 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Tl1	Tl	0.0148	0.0481	0.7536
Mn1	Mn	0.5	0	0	0	1.51	0	1.51
Ni1	Ni	0.5	0	0
Ni2	Ni	0.5	0	0.5	0	0.99	0	0.99
Mn2	Mn	0.5	0	0.5
O1	O	0.8911	0.4484	0.7434
O2	O	0.313	0.2945	0.942
O3	O	0.7076	0.6943	0.4393

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

L. Ding et al. Acta Materialia (2019) · doi:10.1016/j.actamat.2019.04.044

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.291_Tl2NiMnO6.mcif from MAGNDATA · entry page

sha256 of this copy: 34c8da4389cfa0c287ba9ead7f0a84a932dfd8d29e660091e1430f8fa2ca0131
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.291_Tl2NiMnO6.mcif.