Coexistence
of High‑<i>T</i><sub>c</sub> Ferromagnetism and <i>n</i>‑Type Electrical
Conductivity in FeBi<sub>2</sub>Se<sub>4</sub>
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Abstract
The
discovery of <i>n</i>-type ferromagnetic semiconductors
(<i>n</i>-FMSs) exhibiting high electrical conductivity
and Curie temperature (<i>T</i><sub>c</sub>) above 300 K
would dramatically improve semiconductor spintronics and pave the
way for the fabrication of spin-based semiconducting devices. However,
the realization of high-<i>T</i><sub>c</sub> <i>n</i>-FMSs and <i>p</i>-FMSs in conventional high-symmetry semiconductors
has proven extremely difficult due to the strongly coupled and interacting
magnetic and semiconducting sublattices. Here we show that decoupling
the two functional sublattices in the low-symmetry semiconductor FeBi<sub>2</sub>Se<sub>4</sub> enables unprecedented coexistence of high <i>n</i>-type electrical conduction and ferromagnetism with <i>T</i><sub>c</sub> ≈ 450 K. The structure of FeBi<sub>2</sub>Se<sub>4</sub> consists of well-ordered magnetic sublattices
built of [Fe<sub><i>n</i></sub>Se<sub>4<i>n</i>+2</sub>]<sub>∞</sub> single-chain edge-sharing octahedra,
coherently embedded within the three-dimensional Bi-rich semiconducting
framework. Magnetotransport data reveal a negative magnetoresistance,
indicating spin-polarization of itinerant conducting electrons. These
findings demonstrate that decoupling magnetic and semiconducting sublattices
allows access to high-<i>T</i><sub>c</sub> <i>n</i>- and <i>p</i>-FMSs as well as helps unveil the mechanism
of carrier-mediated ferromagnetism in spintronic materials