Research/Sitter/MAGNDATA / 0.732_SrRuO3.mcif

SrRuO₃

MAGNDATA entry 0.732 · 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 ¹m¹m¹m: each symmetry marked ¹ keeps every spin, ² swaps up and down.

ordered ≤ 165 K (−108 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	P n′ m′ a BNS 62.446
Point group	m′m′m
Parent space group	P n m a No. 62
Spins	collinear · net moment 6.52 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 5.52421 · b 7.8348 · c 5.55907 Å · α 90° · β 90° · γ 90°
Transition	165 K (−108 °C)
Measured at	10 K
Magnetic ions	Ru
Largest moment component	1.63 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 n′ m′ a →

Atom sites · 4 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Sr1	Sr	0.4798	0.25	0.4969
Ru1	Ru	0	0	0.5	0	0	1.63	1.63
O1	O	0.504	0.25	−0.0557
O2	O	0.2211	0.4719	0.2218

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.N. Bushmeleva et al. JMMM (2006) · doi:10.1016/j.jmmm.2006.02.089

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.732_SrRuO3.mcif from MAGNDATA · entry page

sha256 of this copy: af36d044962e2ea42cf246a83a4f9e736cf1dab1eaccf04dc980443a10324da3
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.732_SrRuO3.mcif.