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Effect of alloying BaTiO3 with BiZn1/2Ti1/2O3 on polarization reversal
Changes in the polarization state of ferroelectric materials are mediated through the motion of planar defects such as domain walls. The interplay between the two processes that enable the inversion of the macroscopic polarization in ferroelectric materials, non-180° (domain reorientation) and 180°...
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Published in: | Applied physics letters 2020-07, Vol.117 (4) |
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container_title | Applied physics letters |
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creator | Fancher, C. M. Choe, H. Gorfman, S. Simons, H. Chung, C. C. Ziolkowski, M. Prasertpalichat, S. Cann, D. P. Jones, J. L. |
description | Changes in the polarization state of ferroelectric materials are mediated through the motion of planar defects such as domain walls. The interplay between the two processes that enable the inversion of the macroscopic polarization in ferroelectric materials, non-180° (domain reorientation) and 180° (domain reversal), is not well understood. In this work, time-resolved x-ray diffraction was carried out during the application of an external electric field to investigate the dynamic electric-field response mechanisms of BaTiO3 (BT) and BiZn1/2Ti1/2O3(BZT)-modified BT (0.94BT-0.06BZT). These data evidence that the incorporation of BZT into BT fundamentally alters what processes are activated to reorient the polarization by 180°. Polarization reversal in BT is achieved through direct inversion of spontaneous dipoles. However, the addition of BZT into BT promotes a two-step polarization reversal process (i.e., two consecutive non-180° reorientation events). |
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M. ; Choe, H. ; Gorfman, S. ; Simons, H. ; Chung, C. C. ; Ziolkowski, M. ; Prasertpalichat, S. ; Cann, D. P. ; Jones, J. L.</creator><creatorcontrib>Fancher, C. M. ; Choe, H. ; Gorfman, S. ; Simons, H. ; Chung, C. C. ; Ziolkowski, M. ; Prasertpalichat, S. ; Cann, D. P. ; Jones, J. L. ; Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)</creatorcontrib><description>Changes in the polarization state of ferroelectric materials are mediated through the motion of planar defects such as domain walls. The interplay between the two processes that enable the inversion of the macroscopic polarization in ferroelectric materials, non-180° (domain reorientation) and 180° (domain reversal), is not well understood. In this work, time-resolved x-ray diffraction was carried out during the application of an external electric field to investigate the dynamic electric-field response mechanisms of BaTiO3 (BT) and BiZn1/2Ti1/2O3(BZT)-modified BT (0.94BT-0.06BZT). These data evidence that the incorporation of BZT into BT fundamentally alters what processes are activated to reorient the polarization by 180°. Polarization reversal in BT is achieved through direct inversion of spontaneous dipoles. 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In this work, time-resolved x-ray diffraction was carried out during the application of an external electric field to investigate the dynamic electric-field response mechanisms of BaTiO3 (BT) and BiZn1/2Ti1/2O3(BZT)-modified BT (0.94BT-0.06BZT). These data evidence that the incorporation of BZT into BT fundamentally alters what processes are activated to reorient the polarization by 180°. Polarization reversal in BT is achieved through direct inversion of spontaneous dipoles. However, the addition of BZT into BT promotes a two-step polarization reversal process (i.e., two consecutive non-180° reorientation events).</description><subject>Alloying effects</subject><subject>Applied physics</subject><subject>Barium titanates</subject><subject>ceramics</subject><subject>chemical compounds</subject><subject>crystallographic defects</subject><subject>Dipoles</subject><subject>Domain walls</subject><subject>Electric fields</subject><subject>Ferroelectric materials</subject><subject>Ferroelectricity</subject><subject>MATERIALS SCIENCE</subject><subject>perovskites</subject><subject>piezoelectric materials</subject><subject>Polarization</subject><subject>powder diffraction</subject><subject>X-ray diffraction</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNp9kE1LAzEQhoMoWKsH_8GiJ4Vt87Gbj6MtrQqFXurFS8hmszZl3azJtlJ_vakrehC8zPAOD_POOwBcIjhCkJJxPoIQkQzBIzBAkLGUIMSPwQBCSFIqcnQKzkLYRJljQgZgPqsqo7vEVYmqa7e3zUsyUSu7JMm77dbJxD43aIxXNpY4c03Sulp5-6E6G4U3O-ODqs_BSaXqYC6--xA8zWer6UO6WN4_Tu8WqSZIdCllDBXEKJZpjTPGBWGmKLRWushEVXJScpZRJChRhnGssCacobwqqeBc5DkZgqt-rwudlUHbzui1dk0TM0hEM0ExjNB1D7XevW1N6OTGbX0T75I4w5xSdnAYgpue0t6F4E0lW29fld9LBOXhlzKX37-M7G3PHhy_kv_AO-d_QdmW1X_w382f5SN-bQ</recordid><startdate>20200727</startdate><enddate>20200727</enddate><creator>Fancher, C. 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M.</creatorcontrib><creatorcontrib>Choe, H.</creatorcontrib><creatorcontrib>Gorfman, S.</creatorcontrib><creatorcontrib>Simons, H.</creatorcontrib><creatorcontrib>Chung, C. C.</creatorcontrib><creatorcontrib>Ziolkowski, M.</creatorcontrib><creatorcontrib>Prasertpalichat, S.</creatorcontrib><creatorcontrib>Cann, D. P.</creatorcontrib><creatorcontrib>Jones, J. L.</creatorcontrib><creatorcontrib>Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Fancher, C. M.</au><au>Choe, H.</au><au>Gorfman, S.</au><au>Simons, H.</au><au>Chung, C. C.</au><au>Ziolkowski, M.</au><au>Prasertpalichat, S.</au><au>Cann, D. P.</au><au>Jones, J. L.</au><aucorp>Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of alloying BaTiO3 with BiZn1/2Ti1/2O3 on polarization reversal</atitle><jtitle>Applied physics letters</jtitle><date>2020-07-27</date><risdate>2020</risdate><volume>117</volume><issue>4</issue><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>Changes in the polarization state of ferroelectric materials are mediated through the motion of planar defects such as domain walls. The interplay between the two processes that enable the inversion of the macroscopic polarization in ferroelectric materials, non-180° (domain reorientation) and 180° (domain reversal), is not well understood. In this work, time-resolved x-ray diffraction was carried out during the application of an external electric field to investigate the dynamic electric-field response mechanisms of BaTiO3 (BT) and BiZn1/2Ti1/2O3(BZT)-modified BT (0.94BT-0.06BZT). These data evidence that the incorporation of BZT into BT fundamentally alters what processes are activated to reorient the polarization by 180°. Polarization reversal in BT is achieved through direct inversion of spontaneous dipoles. 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subjects | Alloying effects Applied physics Barium titanates ceramics chemical compounds crystallographic defects Dipoles Domain walls Electric fields Ferroelectric materials Ferroelectricity MATERIALS SCIENCE perovskites piezoelectric materials Polarization powder diffraction X-ray diffraction |
title | Effect of alloying BaTiO3 with BiZn1/2Ti1/2O3 on polarization reversal |
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