Research/Sitter/MAGNDATA / 0.423_EuMnSb2.mcif

EuMnSb₂

MAGNDATA entry 0.423 · source

antiferromagnet

No net magnetisation, and up and down sublattices are related by a shift or by inversion, so the bands stay spin-degenerate: a conventional antiferromagnet.

Spin group ¹m¹m¹m × ²1: each symmetry marked ¹ keeps every spin, ² swaps up and down.

ordered ≤ 346 K (73 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 10 properties

Magnetic group	P n′ m′ a′ BNS 62.449
Parent space group	P n m a No. 62
Spins	collinear · net moment 0 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 22.5726 · b 4.385 · c 4.4095 Å · α 90° · β 90° · γ 90°
Transition	346 K (73 °C)
Measured at	150 K
Magnetic ions	Eu, Mn
Largest moment component	4 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 n′ m′ a′ →

Atom sites · 4 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Eu1	Eu	0.3864	0.25	0.7698
Mn1	Mn	0.2497	0.25	0.2701	4	0	0	4
Sb1	Sb	0.1747	0.25	0.7701
Sb2	Sb	0.499	0.25	0.2782

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

D. Gong et al. PHYSICAL REVIEW B (2020) · doi:10.1103/PhysRevB.101.224422

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.423_EuMnSb2.mcif from MAGNDATA · entry page

sha256 of this copy: 5d40c12331e880f80f9c3ec9e91a90325197120c60968d5a899077bb7dd0883a
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.423_EuMnSb2.mcif.