Research/Sitter/MAGNDATA / 0.490_YbMnO3.mcif

YbMnO₃

MAGNDATA entry 0.490 · source

noncoplanar ferrimagnet

Opposite moments of different size leave a net magnetisation.

ordered ≤ 5 K (−268 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 10 properties

Magnetic group	P 6₃ c′ m′ BNS 185.201
Parent space group	P 6₃ c m No. 185
Spins	noncoplanar · net moment 4.1 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 6.0584 · b 6.0584 · c 11.3561 Å · α 90° · β 90° · γ 120°
Transition	5 K (−268 °C)
Measured at	2 K
Magnetic ions	Mn, Yb
Largest moment component	3.41 μ_B
Method	NSD

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 6₃ c′ m′ →

Atom sites · 7 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Yb1	Yb	0	0	0.2734	0	0	−1.47	1.47
Yb2	Yb	0.3333	0.6667	0.2306	0	0	1.76	1.76
Mn1	Mn	0.3349	0	0	3.41	0	0	3.41
O1	O	0.303	0	0.1617
O2	O	0.361	0	0.8342
O3	O	0	0	0.9732
O4	O	0.3333	0.6667	0.0192

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

S. Chattopadhyay et al. PHYSICAL REVIEW B (2018) · doi:10.1103/PhysRevB.98.134413

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.490_YbMnO3.mcif from MAGNDATA · entry page

sha256 of this copy: aee4807b141be8319c7763dc330beec7f0919c0492b679182bab468654c333ae
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.490_YbMnO3.mcif.