Research/Sitter/MAGNDATA / 0.738_LaBaMn2O6.mcif

LaBaMn₂O₆

MAGNDATA entry 0.738 · 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 ≤ 335 K (62 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	P 4/m m′ m′ BNS 123.345
Point group	4/mm′m′
Parent space group	P 4/m m m No. 123
Spins	collinear · net moment 2.574 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 3.909 · b 3.909 · c 7.7958 Å · α 90° · β 90° · γ 90°
Transition	335 K (62 °C)
Measured at	293 K
Magnetic ions	Mn
Largest moment component	1.287 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/m m′ m′ →

Atom sites · 6 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
La1	La	0	0	0
Ba1	Ba	0	0	0.5
Mn1	Mn	0.5	0.5	0.2519	0	0	1.287	1.287
O1	O	0	0.5	0.2649
O2	O	0.5	0.5	0
O3	O	0.5	0.5	0.5

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

F. Millange et al. Chem. Mater. (1998) · doi:10.1021/cm980130v

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.738_LaBaMn2O6.mcif from MAGNDATA · entry page

sha256 of this copy: 0d8477ad566b3aeaf0e78a281cd436b3439d2452ee76f4b1149357e94969b65d
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.738_LaBaMn2O6.mcif.