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    Electrodeposition of Co<sub><i>x</i></sub>Fe<sub>3–<i>x</i></sub>O<sub>4</sub> Epitaxial Films and Superlattices

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    Spinel ferrites are of interest because of their potential applications in spintronics (spin-based electronics) and solid-state memories. Cobalt ferrite (CoFe<sub>2</sub>O<sub>4</sub>) is an inverse spinel ferrite. Currently, the utility of CoFe<sub>2</sub>O<sub>4</sub> is mainly based on its high coercivity and magnetocrystalline anisotropy. The magnetic and electrical properties of CoFe<sub>2</sub>O<sub>4</sub> depend on its Co:Fe ratio. In this paper, a one-step electrodeposition of Co<sub><i>x</i></sub>Fe<sub>3‑x</sub>O<sub>4</sub> (0 < <i>x</i> < 1) thin films from an alkaline Fe<sup>3+</sup>- and Co<sup>2+</sup>-triethanolamine solution is presented. The Co:Fe ratio in the Co<sub><i>x</i></sub>Fe<sub>3–<i>x</i></sub>O<sub>4</sub> thin films can be tuned by controlling the deposition potential. That is, Co<sub><i>x</i></sub>Fe<sub>3–<i>x</i></sub>O<sub>4</sub> thin films with tunable chemical and physical properties can be produced from a single solution. Superlattices in the Co<sub><i>x</i></sub>Fe<sub>3–<i>x</i></sub>O<sub>4</sub> system were also electrodeposited from the same solution by simply pulsing between two potentials. Compared to Co<sub><i>x</i></sub>Fe<sub>3–<i>x</i></sub>O<sub>4</sub> individual films, superlattices exhibit resistance switching and a more pronounced negative differential resistance (NDR) feature at lower current during perpendicular transport measurements, which could be used in resistive random access memories
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