Research/Sitter/MAGNDATA / 1.16_BaFe2As2.mcif

BaFe₂As₂

MAGNDATA entry 1.16 · 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 ≤ 142 K (−131 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	C_A m c a BNS 64.480
Point group	mmm1′
Parent space group	I 4/m m m No. 139
Spins	collinear · net moment 0 μ_B per cell
Propagation	[1/2 1/2 0] 1k
Cell	a 12.9428 · b 5.61587 · c 5.57125 Å · α 90° · β 90° · γ 90°
Transition	142 K (−131 °C)
Measured at	5 K
Magnetic ions	Fe
Largest moment component	0.87 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 C_A m c a →

Atom sites · 3 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Ba	Ba	0	0	0
Fe	Fe	0.25	0.25	0.25	0	0.87	0	0.87
As	As	0.3541	0	0

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

Q. Huang et al. Phys. Rev. Lett. (2008) · doi:10.1103/physrevlett.101.257003

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 1.16_BaFe2As2.mcif from MAGNDATA · entry page

sha256 of this copy: 0ae8598ccc1eec4b9d6a3c90f5c5e699ee40d47501b4114d0623224cd74a46b0
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 1.16_BaFe2As2.mcif.