Structure and Dynamics of Ferroelectric Domains in Polycrystalline Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>
A complex domain structure with variations in the morphology is observed at ambient temperature in monoclinic Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>. Using electron microscopy and piezoresponse force microscopy, it is possible to reveal micrometre-sized...
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doaj-442a9ff58ed9471db08294665f6b7d8f2020-11-24T21:52:16ZengMDPI AGMaterials1996-19442019-04-01128132710.3390/ma12081327ma12081327Structure and Dynamics of Ferroelectric Domains in Polycrystalline Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>Hana Ursic0Andreja Bencan1Uros Prah2Mirela Dragomir3Barbara Malic4Electronic Ceramics Department, Jozef Stefan Institute, Jamova cesta 39, 1000 Ljubljana, SloveniaElectronic Ceramics Department, Jozef Stefan Institute, Jamova cesta 39, 1000 Ljubljana, SloveniaElectronic Ceramics Department, Jozef Stefan Institute, Jamova cesta 39, 1000 Ljubljana, SloveniaElectronic Ceramics Department, Jozef Stefan Institute, Jamova cesta 39, 1000 Ljubljana, SloveniaElectronic Ceramics Department, Jozef Stefan Institute, Jamova cesta 39, 1000 Ljubljana, SloveniaA complex domain structure with variations in the morphology is observed at ambient temperature in monoclinic Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>. Using electron microscopy and piezoresponse force microscopy, it is possible to reveal micrometre-sized wedge, lamellar-like, and irregularly shaped domains. By increasing the temperature, the domain structure persists up to 80 °C, and then starts to disappear at around 100 °C due to the proximity of the ferroelectric–paraelectric phase transition, in agreement with macroscopic dielectric measurements. In order to understand to what degree domain switching can occur in the ceramic, the mobility of the domain walls was studied at ambient temperature. The in situ poling experiment performed using piezoresponse force microscopy resulted in an almost perfectly poled area, providing evidence that all types of domains can be easily switched. By poling half an area with 20 V and the other half with −20 V, two domains separated by a straight domain wall were created, indicating that Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub> is a promising material for domain-wall engineering.https://www.mdpi.com/1996-1944/12/8/1327Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>ferroelectric domainpiezoresponse force microscopymonoclinic phase |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Hana Ursic Andreja Bencan Uros Prah Mirela Dragomir Barbara Malic |
spellingShingle |
Hana Ursic Andreja Bencan Uros Prah Mirela Dragomir Barbara Malic Structure and Dynamics of Ferroelectric Domains in Polycrystalline Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub> Materials Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub> ferroelectric domain piezoresponse force microscopy monoclinic phase |
author_facet |
Hana Ursic Andreja Bencan Uros Prah Mirela Dragomir Barbara Malic |
author_sort |
Hana Ursic |
title |
Structure and Dynamics of Ferroelectric Domains in Polycrystalline Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub> |
title_short |
Structure and Dynamics of Ferroelectric Domains in Polycrystalline Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub> |
title_full |
Structure and Dynamics of Ferroelectric Domains in Polycrystalline Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub> |
title_fullStr |
Structure and Dynamics of Ferroelectric Domains in Polycrystalline Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub> |
title_full_unstemmed |
Structure and Dynamics of Ferroelectric Domains in Polycrystalline Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub> |
title_sort |
structure and dynamics of ferroelectric domains in polycrystalline pb(fe<sub>1/2</sub>nb<sub>1/2</sub>)o<sub>3</sub> |
publisher |
MDPI AG |
series |
Materials |
issn |
1996-1944 |
publishDate |
2019-04-01 |
description |
A complex domain structure with variations in the morphology is observed at ambient temperature in monoclinic Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub>. Using electron microscopy and piezoresponse force microscopy, it is possible to reveal micrometre-sized wedge, lamellar-like, and irregularly shaped domains. By increasing the temperature, the domain structure persists up to 80 °C, and then starts to disappear at around 100 °C due to the proximity of the ferroelectric–paraelectric phase transition, in agreement with macroscopic dielectric measurements. In order to understand to what degree domain switching can occur in the ceramic, the mobility of the domain walls was studied at ambient temperature. The in situ poling experiment performed using piezoresponse force microscopy resulted in an almost perfectly poled area, providing evidence that all types of domains can be easily switched. By poling half an area with 20 V and the other half with −20 V, two domains separated by a straight domain wall were created, indicating that Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub> is a promising material for domain-wall engineering. |
topic |
Pb(Fe<sub>1/2</sub>Nb<sub>1/2</sub>)O<sub>3</sub> ferroelectric domain piezoresponse force microscopy monoclinic phase |
url |
https://www.mdpi.com/1996-1944/12/8/1327 |
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