Ferroelectric Behavior of PZT-BCO-BFO Solid Solutions
ORAL
Abstract
The ferroelectric behavior of 75% PbZr0.5Ti0.5O3 - 25% BiMO3 (where M=Fe,Co) (PZT-BMO) was studied using first principles density functional theory calculations. Despite the large rhombohedral and tetragonal polar distortions expected for the BiFeO3 (BFO) and
BiCoO3 (BCO) end members, respectively, we find that both solid solutions retain the monoclinic phase of PZT. Furthermore, unlike the BCO and BFO end members that have large polarizations, the polarization for the PZT-BCO solid solution was determined to be 0.6 C/m2, closer to that of PZT. Combining our results with previous work on the BCO-BFO solid solution, we are able to suggest a phase diagram where PZT rich compositions retain the monoclinic phase present at the morphotropic phase boundary in PZT. Together, these results suggest the possibility of enhanced electromechanical responses for compositions of PZT-BMO with less than 75% PZT; thereby providing a novel route to designing high performance piezoelectrics with reduced Pb content.
BiCoO3 (BCO) end members, respectively, we find that both solid solutions retain the monoclinic phase of PZT. Furthermore, unlike the BCO and BFO end members that have large polarizations, the polarization for the PZT-BCO solid solution was determined to be 0.6 C/m2, closer to that of PZT. Combining our results with previous work on the BCO-BFO solid solution, we are able to suggest a phase diagram where PZT rich compositions retain the monoclinic phase present at the morphotropic phase boundary in PZT. Together, these results suggest the possibility of enhanced electromechanical responses for compositions of PZT-BMO with less than 75% PZT; thereby providing a novel route to designing high performance piezoelectrics with reduced Pb content.
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Presenters
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David Parker
Oak Ridge National Laboratory, Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge National Lab
Authors
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David Parker
Oak Ridge National Laboratory, Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge National Lab
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Simuck Yuk
Materials Science and Technology Division, Oak Ridge National Laboratory
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Valentino Cooper
Oak Ridge National Lab, Oak Ridge National Laboratory, Materials Science & Technology Division, Oak Ridge National Lab, Materials Science and Technology Division, Oak Ridge National Lab, ORNL, Materials Science and Technology Division, Oak Ridge National Laboratory