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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Alexe, Marin
Max Planck Institute of Microstructure Physics
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (8/8 displayed)
- 2022Enhanced photoconductivity at dislocations in SrTiO 3citations
- 2016Physical aspects of ferroelectric semiconductors for photovoltaic solar energy conversioncitations
- 2016Description of domain wall motions by the hyperbolic law
- 2013Nucleation-Induced Self-Assembly of Multiferroic BiFeO3-CoFe2O4 Nanocompositescitations
- 2006Threading dislocations in epitaxial ferroelectric PbZr0.2Ti0.8O3 films and their effect on polarization backswitchingcitations
- 2005High-resolution electron energy-loss spectroscopy of Ba Ti O 3∕ Sr Ti O 3 multilayerscitations
- 2002Initial growth stages of epitaxial BaTiO3 films on vicinal SrTiO3 (001) substrate surfacescitations
- 2002Initial growth stages of epitaxial BaTiO3 films on vicinal SrTiO3 : Nb (001) substrates
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document
Description of domain wall motions by the hyperbolic law
Abstract
In ferroelectric materials, domain walls interact with lattice defects and several types of domain walls displacements can be observed. When a domain wall is trapped at a pinning point, it can “jump” to another pinning center only if the driving electric field is sufficiently high. On the contrary, if the field is too weak, the domain wall only vibrates around its equilibrium position. Thus, both situations contribute to the value of the permittivity which can be described by the hyperbolic law. This law is based on reversible and irreversible domain wall motions and allows us to dissociate the domain wall and lattice contributions from the dielectric measurements.