We prepared a new polar layered quantum magnet Ba2Cu3(SeO3)4F2,
by a combined
use of F– and pyramidal SeO3
2– anions, determined its crystal structure by X-ray diffraction, and
characterized its magnetic properties by magnetization, electron spin
resonance (ESR) and specific heat measurements, and by density functional
theory calculations. The title compound has first experimentally reported
bitriangular chains of Cu2+ ions aligned along the b direction to form layers parallel to the ab plane, and these layers are separated by Ba2+ ions. The
magnetic susceptibility data reveal that, despite strong predominant
antiferromagnetic intrachain interactions indicated by the large negative
Weiss temperature θ of −143.9 K within bitriangular chains,
no long-range order occurs down to 2 K. The latter, further confirmed
by the specific heat measurements, is attributed to the extremely
weak interlayer interaction. The spins in each bitriangular chain
become ferrimagnetically ordered to exhibit a 1/3-magnetization plateau,
which persists at least up to 30 T. This reveals that each bitriangular
chain acts as an S = 1/2 entity at low temperatures,
as observed from the decrease of the effective magnetic moment P
eff from 3.67 μB in the high
temperature range to 1.89 μB in the low temperature
range, equivalently, from three free Cu2+ ions to only
one effective Cu2+ ion per formula unit. In each layer
of Ba2Cu3(SeO3)4F2, the interaction between adjacent ferrimagnetic chains is
ferromagnetic rather than antiferromagnetic, contrary to the observations
in other reported cases.