Research/Sitter/MAGNDATA / 0.1190_CuCoFe2O5.mcif

CuCoFe₂O₅

MAGNDATA entry 0.1190 · source

noncollinear ferrimagnet

Opposite moments of different size leave a net magnetisation.

ordered ≤ 195 K (−78 °C)Colour: where that sits relative to 25 °C. Saturation: how much margin it has.

Structure · 11 properties

Magnetic group	C m′ c′ m BNS 63.462
Point group	m′m′m
Parent space group	C m c m No. 63
Spins	coplanar · net moment 10.8 μ_B per cell
Propagation	[0 0 0] 1k
Cell	a 2.8866 · b 9.7493 · c 12.5235 Å · α 90° · β 90° · γ 90°
Transition	195 K (−78 °C)
Measured at	90 K
Magnetic ions	Co, Cu, Fe
Largest moment component	2.5 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 m′ c′ m →

Atom sites · 10 sites · CSV

site	element	x	y	z	m_a	m_b	m_c	\|m\| (μ_B)
Cu1	Cu	0	0.5175	0.226	0	0	−1.3	1.3
Co1	Co	0	0.5175	0.226	0	0	−1.3	1.3
Co2	Co	0	0	0	0	1.3	−2.5	2.8178
Cu2	Cu	0	0	0	0	1.3	−2.5	2.8178
Fe2	Fe	0	0	0	0	1.3	−2.5	2.8178
Fe3	Fe	0.5	0.7615	0.1149	0	−1.3	2.5	2.8178
Co3	Co	0.5	0.7615	0.1149	0	−1.3	2.5	2.8178
O1	O	0.5	0.665	0.75
O2	O	0	0.0986	0.1409
O3	O	0.5	−0.147	0.0479

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

Leelashree Solaiappan et al. Chem. Mater. (2026) · doi:10.1021/acs.chemmater.6c00764

Cite the original paper and MAGNDATA, not this mirror.

Original file

⬇ 0.1190_CuCoFe2O5.mcif from MAGNDATA · entry page

sha256 of this copy: ab648e2bfcc19660bd78c90e2d20fc00eb2c4fb31bd0a03936997822658fb8fa
The mirror keeps the bytes Bilbao served, so the original should hash the same unless MAGNDATA has revised the entry since: shasum -a 256 0.1190_CuCoFe2O5.mcif.