CONICET | Buscador de Institutos y Recursos Humanos

Noble/transition bimetallic nanowires of nominal composition FexRh100-x (x = 15, 25, 54) are AC electrodeposited into 20 nm diameter hexagonally self-assembled nanopores of anodic alumina membranes. Nanowires about 18 nm in diameter and 1 μm long are polycrystalline and, depending on composition, different crystalline phases are obtained. Iron-rich (x = 54) wires are biphasic, composed by large α-Fe grains (>100 nm in length) and clusters of small (3 nm in average) grains of fcc γ-Rh(Fe) phase, with composition near (30 ± 5) at% Fe. Rh-rich (x = 15, 25) nanowires are formed by very small grains of γ-Rh(Fe) phase. Grain size depends on Rh content: grains in wires with x = 15 are the smallest with a mean size of (2.1 ± 0.9) nm. The low temperature magnetic properties of these small grained nanowires exhibit new features: they are all ferromagnetic at 5 K while, at room temperature wires with 54 at.% Fe and 25 at.% Fe are ferromagnetic and those with 15 at.% Fe are weakly superparamagnetic. These behaviors are consistent with non-compensated and very small ferrimagnetic grains surrounded by a grain boundary disordered spin-glass-like phase that freezes below 40 K. This frozen intergranular phase favors a strong exchange coupling between the ferrimagnetic grains, which undergo a cooperative, ferromagnetic-like behavior under an external magnetic field. Above 40 K nanowires with 54 at.% Fe are ferromagnetic and those containing 25 at.% Fe exhibit a ferromagnetic-like behavior arising from blocked antiferromagnetic grains. Nanowires 15 at.% Fe are weakly superparamagnetic above 40 K. Arrays containing 54 at.% Fe and 25 at.% Fe exhibit a polarization reversal mechanism involving localized nucleation and further expansion of inverse domains; this thermally activated, magnetic field assisted mechanism exhibits an apparent activation energy between 229 kJ/mol (2.3 eV) and 298 kJ/mol (3.1 eV) for nanowires 25 at.% Fe and 54 at.% Fe, respectively.