Abstract

Multiferroic materials have attracted much interest due to the unusual coexistence of ferroelectric and (anti-)ferromagnetic ground states in a single compound. They offer an exciting platform for new physics and potentially novel devices. BiFeO3_3 is one of the most celebrated of multiferroic materials with highly desirable properties. It is the only known room-temperature multiferroic with TC≈1100 KT_\mathrm{C}\approx 1100~ \mathrm{K} and TN≈650 KT_\mathrm{N}\approx 650~\mathrm{K}, and exhibits one of the largest spontaneous electric polarisation, P≈80 μC/cm2P\approx 80~μ\mathrm{C/cm}^2. At the same time, it has a magnetic cycloid structure with an extremely long period of 630~Å, which arises from a competition between the usual symmetric exchange interaction and antisymmetric Dzyaloshinskii-Moriya (DM) interaction. There is also an intriguing interplay between the DM interaction and the single ion anisotropy. In this review, we have tried to paint a complete picture of bulk BiFeO3_3 by summarising the structural and dynamical properties of both spin and lattice parts, and their magneto-electric coupling.

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