Research/Sitter/MAGNDATA / 0.10_DyFeO3.mcif

DyFeO₃

MAGNDATA entry 0.10 · 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 ≤ 4 K (−269 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 10 properties

Magnetic group	P 2₁2₁2₁ BNS 19.25
Point group	222
Parent space group	P n m a No. 62
Spins	coplanar · net moment 0 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 5.5957 · b 7.629 · c 5.3009 Å · α 90° · β 90° · γ 90°
Transition	4 K (−269 °C)
Magnetic ions	Dy, Fe
Largest moment component	1 μ_B
Method	arbitrary spin values

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 2₁2₁2₁ →

Atom sites · 5 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Dy1	Dy	0.0667	0.25	0.9828	1	0	0	1
Fe1	Fe	0	0	0.5	1	0.3	0	1.044
O1	O	0.4626	0.25	0.1081
O2_1	O	0.6967	0.9443	0.3075
O2_2	O	0.3033	0.0557	0.6925

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

Y. Tokunaga et al. Phys. Rev. Lett. (2008) · doi:10.1103/physrevlett.101.097205

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.10_DyFeO3.mcif from MAGNDATA · entry page

sha256 of this copy: d5c56ccfa23fc12dc98cc86034c71e09eb904e78d23c2db5cab6d9c4d82abded
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.10_DyFeO3.mcif.