A Room‐Temperature Ferroelectric Ferromagnet in a 1D Tetrahedral Chain Network
Ferroelectricity occurs in crystals with broken spatial inversion symmetry. In conventional perovskite oxides, concerted ionic displacements within a 3D network of transition‐metal–oxygen polyhedra (MOx) manifest spontaneous polarization. Meanwhile, some 2D networks of MOx foster geometric ferroelec...
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Veröffentlicht in: | Advanced materials (Weinheim) 2019-06, Vol.31 (24), p.e1808104-n/a |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Ferroelectricity occurs in crystals with broken spatial inversion symmetry. In conventional perovskite oxides, concerted ionic displacements within a 3D network of transition‐metal–oxygen polyhedra (MOx) manifest spontaneous polarization. Meanwhile, some 2D networks of MOx foster geometric ferroelectricity with magnetism, owing to the distortion of the polyhedra. Because of the fundamentally different mechanism of ferroelectricity in a 2D network, one can further challenge an uncharted mechanism of ferroelectricity in a 1D channel of MOx and estimate its feasibility. Here, ferroelectricity and coupled ferromagnetism in a 1D FeO4 tetrahedral chain network of a brownmillerite SrFeO2.5 epitaxial thin film are presented. The result provides a new paradigm for designing low‐dimensional MOx networks, which is expected to benefit the realization of macroscopic ferro‐ordering materials including ferroelectric ferromagnets.
A new class of room‐temperature ferroelectric ferromagnet in a 1D tetrahedral network is presented. Compared to the conventional ferroelectrics of 3D and 2D polyhedral networks, 1D tetrahedral networks exhibit an uncharted physical mechanism, which is the combined polar distortion for ferro‐orderings. Engineering polyhedral networks in 1D unveils novel pathways to design and realize functionalities in transition‐metal oxides. |
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ISSN: | 0935-9648 1521-4095 |
DOI: | 10.1002/adma.201808104 |