Research/Sitter/MAGNDATA / 0.593_UPSe.mcif

UPSe

MAGNDATA entry 0.593 · 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 ¹4/¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.

ordered ≤ 110 K (−163 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 10 properties

Magnetic group	P 4/n m′ m′ BNS 129.417
Parent space group	P 4/n m m No. 129
Spins	collinear · net moment 2.7 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 3.951 · b 3.951 · c 8.185 Å · α 90° · β 90° · γ 90°
Transition	110 K (−163 °C)
Measured at	4 K
Magnetic ions	U
Largest moment component	1.35 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 4/n m′ m′ →

Atom sites · 3 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
U1	U	0.25	0.25	0.261	0	0	1.35	1.35
Se1	Se	0.25	0.25	0.6435
P1	P	0.75	0.25	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

A. Zygmunt et al. phys. stat. sol. (a) (1974) · doi:10.1002/pssa.2210250155

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.593_UPSe.mcif from MAGNDATA · entry page

sha256 of this copy: 2479730129c0756fea2ed027328eab1664f36971896a339d40bec0185464e622
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.593_UPSe.mcif.