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Journal article

Dynamics and grain orientation dependence of the electric field induced phase transformation in Sm modified BiFeO3 ceramics

From

Department of Physics, Technical University of Denmark1

Neutrons and X-rays for Materials Physics, Department of Physics, Technical University of Denmark2

Josef Stefan Institute3

The European Synchrotron4

Pennsylvania State University5

Samarium-modified bismuth ferrite ((Bi,Sm)FeO3 or BSFO) is a room-temperature multiferroic with a morphotropic phase boundary near 15.5 mol% Sm, where ferroelectric, antiferroelectric and paraelectric phases coexist and the electromechanical response (Smax/Emax and d33) is maximized. Recently, an electric field induced phase transformation was discovered, which is believed to play a significant role in the macroscopic electromechanical response.

Here, we used in situ synchrotron X-ray powder diffraction to directly measure this transformation in real time within bulk ceramics to determine the dynamics, structural pathway and crystallographic orientation dependence of the transformation. Our results show that there are two transformation pathways; an antiferroelectric-to-ferroelectric transformation, which is revesible, and a paraelectric-to-ferroelectric transformation, which is irreversible.

Furthermore, these transformations occur with a strong orientation dependence with respect to the applied electric field direction, and with extremely slow dynamics - just 2 to 10 minutes - orders of magnitude longer than in other ferroelectrics (e.g. Bi1/2Na1/2TiO3-BaTiO3 or BNT-BT). These findings point to texturing and the elimination of the paraelectric phase to enhance the electromechanical response.

Moreover, they provide a detailed picture of the transformation dynamics and a greater understanding of electric field induced transformations in ferroelectric ceramics.

Language: English
Year: 2018
Pages: 7635-7641
ISSN: 20507534 and 20507526
Types: Journal article
DOI: 10.1039/c8tc01951g
ORCIDs: 0000-0001-8193-4232 , 0000-0002-7780-6710 and 0000-0002-3093-9241

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