Research/Sitter/MAGNDATA / 0.534_Tb0.55Sr0.45MnO3.mcif

Tb_0.55Sr_0.45MnO₃

MAGNDATA entry 0.534 · source

noncoplanar ferrimagnet

Opposite moments of different size leave a net magnetisation.

ordered ≤ 8 K (−265 °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 62.447
Parent space group	P n m a No. 62
Spins	noncoplanar · net moment 2.52 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 5.408 · b 7.611 · c 5.392 Å · α 90° · β 90° · γ 90°
Transition	8 K (−265 °C)
Measured at	1.5 K
Magnetic ions	Mn, Tb
Largest moment component	1.43 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 · 5 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Tb1	Tb	0.9685	0.25	0.0049	0.41	0	1.43	1.4876
Sr1	Sr	0.9685	0.25	0.0049
Mn1	Mn	0	0	0.5	0.22	0.45	−0.52	0.722
O1	O	0.0138	0.25	0.5656
O2	O	0.718	0.4648	0.2804

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

H. Agarwal et al. Journal of Alloys and Compounds (2020) · doi:10.1016/j.jallcom.2020.156355

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.534_Tb0.55Sr0.45MnO3.mcif from MAGNDATA · entry page

sha256 of this copy: 60b723707d775d0c367902da19874eb3fd24070b30c182b146d2c039fe21e173
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.534_Tb0.55Sr0.45MnO3.mcif.