Abstract
Ferroelectric materials exhibit the largest dielectric permittivities and piezoelectric responses in nature, making them invaluable in applications from supercapacitors or sensors to actuators or electromechanical transducers. The origin of this behavior is their proximity to phase transitions. However, the largest possible responses are most often not utilized due to the impracticality of using temperature as a control parameter and to operate at phase transitions. This has motivated the design of solid solutions with morphotropic phase boundaries between different polar phases that are tuned by composition and that are weakly dependent on temperature. Thus far, the best piezoelectrics have been achieved in materials with intermediate (bridging or adaptive) phases. But so far, complex chemistry or an intricate microstructure has been required to achieve temperature-independent phase-transition boundaries. Here, we report such a temperature-independent bridging state in thin films of chemically simple BaTiO3. A coexistence among tetragonal, orthorhombic, and their bridging low-symmetry phases are shown to induce continuous vertical polarization rotation, which recreates a smear in-transition state and leads to a giant temperature-independent dielectric response. The current material contains a ferroelectric state that is distinct from those at morphotropic phase boundaries and cannot be considered as ferroelectric crystals. We believe that other materials can be engineered in a similar way to contain a ferroelectric state with gradual change of structure, forming a class of transitional ferroelectrics. Similar mechanisms could be utilized in other materials to design low-power ferroelectrics, piezoelectrics, dielectrics, or shape-memory alloys, as well as efficient electro- and magnetocalorics.
Original language | English |
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Article number | 011402 |
Journal | Applied Physics Reviews |
Volume | 7 |
Issue number | 1 |
DOIs | |
State | Published - Mar 1 2020 |
Externally published | Yes |
Funding
The authors are grateful to U. Bhaskar for preliminary piezoelectric measurements, to C. Magén for preliminary TEM measurements, to G. Agnus for developing oxides patterning processes, and to N. Robin, P. Muralt, and D. Damjanovic for useful discussions. A.S.E. and B.N. acknowledge financial support from the alumni organization of the University of Groningen, De-Aduarderking (Ubbo Emmius Fonds), and from the Zernike Institute for Advanced Materials. T.D. acknowledges the European Metrology Research Programme (EMRP) Project No. IND54 397 Nanostrain and the European Union's Seventh Framework Programme (No. FP7/2007-2013)/ERC Grant Agreement No. 320832. T.D. thanks Knut Müller-Caspary for technical help with the STEM experiment. A.G. acknowledges funding by the Deutsche Forschungsgemeinschaft (Nos. SPP 1599 GR 4792/1-2 and GR 4792/2-1). Y.T.S. and J.M.Z. acknowledge the financial support by the DOE BES (Grant No. DEFG02-01ER45923). Electron diffraction experiments were carried out at the Center for Microanalysis of Materials at the Frederick Seitz Materials Research Laboratory of the University of Illinois at Urbana-Champaign. J.H. and P.O. were supported by the Operational Programme Research, Development, and Education (financed by European Structural and Investment Funds and by the Czech Ministry of Education, Youth, and Sports), Project No. SOLID21-CZ.02.1.01/0.0/0.0/16_019/0000760). N.D. and G.C. acknowledge financial support by the Severo Ochoa Excellence programme.
Funders | Funder number |
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Czech Ministry of Education, Youth, and Sports | SOLID21-CZ.02.1.01/0.0/0.0/16_019/0000760 |
Zernike Institute for Advanced Materials | |
Basic Energy Sciences | DEFG02-01ER45923 |
Seventh Framework Programme | 320832 |
European Metrology Programme for Innovation and Research | |
European Research Council | |
Deutsche Forschungsgemeinschaft | GR 4792/2-1, SPP 1599 GR 4792/1-2 |
Rijksuniversiteit Groningen | |
Seventh Framework Programme | FP7/2007-2013 |