Strain-gradient-induced electric polarization in lead zirconate titanate ceramics
Strain-gradient-induced polarization or flexoelectricity was investigated in unpoled soft lead zirconate titanate (PZT) ceramic where the texture symmetry m∞∞ forbids macropiezoelectricity. Even under high strain gradient (1 m−1) the induced polarization is small (1.6 μC/m2) at 20 °C. Higher strain...
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Veröffentlicht in: | Applied physics letters 2003-05, Vol.82 (19), p.3293-3295 |
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description | Strain-gradient-induced polarization or flexoelectricity was investigated in unpoled soft lead zirconate titanate (PZT) ceramic where the texture symmetry m∞∞ forbids macropiezoelectricity. Even under high strain gradient (1 m−1) the induced polarization is small (1.6 μC/m2) at 20 °C. Higher strain gradients induce ferroelastic poling and an additional extrinsic contribution to the flexoelectric coefficient μ12 raising the value from 0.5 to 2.0 μC/m. Cooling through the Curie point (TC) under maximum stress (80 MPa) where the peak permittivity (∼20 000) could raise μ12 to 20 μC/m, the equivalent electric field is still only ∼1 kV/m, inadequate to achieve significant ferroelectric poling. The situation may be different in thin PZT films where much larger strain gradients can occur. |
doi_str_mv | 10.1063/1.1570517 |
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Eric</creator><creatorcontrib>Ma, Wenhui ; Cross, L. Eric</creatorcontrib><description>Strain-gradient-induced polarization or flexoelectricity was investigated in unpoled soft lead zirconate titanate (PZT) ceramic where the texture symmetry m∞∞ forbids macropiezoelectricity. Even under high strain gradient (1 m−1) the induced polarization is small (1.6 μC/m2) at 20 °C. Higher strain gradients induce ferroelastic poling and an additional extrinsic contribution to the flexoelectric coefficient μ12 raising the value from 0.5 to 2.0 μC/m. Cooling through the Curie point (TC) under maximum stress (80 MPa) where the peak permittivity (∼20 000) could raise μ12 to 20 μC/m, the equivalent electric field is still only ∼1 kV/m, inadequate to achieve significant ferroelectric poling. The situation may be different in thin PZT films where much larger strain gradients can occur.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/1.1570517</identifier><language>eng</language><ispartof>Applied physics letters, 2003-05, Vol.82 (19), p.3293-3295</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c293t-3c1c3eba430dbca8dccdf3fd0915c68e227f078f44391d9b363cbe9ab09c310e3</citedby><cites>FETCH-LOGICAL-c293t-3c1c3eba430dbca8dccdf3fd0915c68e227f078f44391d9b363cbe9ab09c310e3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Ma, Wenhui</creatorcontrib><creatorcontrib>Cross, L. Eric</creatorcontrib><title>Strain-gradient-induced electric polarization in lead zirconate titanate ceramics</title><title>Applied physics letters</title><description>Strain-gradient-induced polarization or flexoelectricity was investigated in unpoled soft lead zirconate titanate (PZT) ceramic where the texture symmetry m∞∞ forbids macropiezoelectricity. Even under high strain gradient (1 m−1) the induced polarization is small (1.6 μC/m2) at 20 °C. Higher strain gradients induce ferroelastic poling and an additional extrinsic contribution to the flexoelectric coefficient μ12 raising the value from 0.5 to 2.0 μC/m. Cooling through the Curie point (TC) under maximum stress (80 MPa) where the peak permittivity (∼20 000) could raise μ12 to 20 μC/m, the equivalent electric field is still only ∼1 kV/m, inadequate to achieve significant ferroelectric poling. 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Eric</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c293t-3c1c3eba430dbca8dccdf3fd0915c68e227f078f44391d9b363cbe9ab09c310e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2003</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Ma, Wenhui</creatorcontrib><creatorcontrib>Cross, L. Eric</creatorcontrib><collection>CrossRef</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Ma, Wenhui</au><au>Cross, L. Eric</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Strain-gradient-induced electric polarization in lead zirconate titanate ceramics</atitle><jtitle>Applied physics letters</jtitle><date>2003-05-12</date><risdate>2003</risdate><volume>82</volume><issue>19</issue><spage>3293</spage><epage>3295</epage><pages>3293-3295</pages><issn>0003-6951</issn><eissn>1077-3118</eissn><abstract>Strain-gradient-induced polarization or flexoelectricity was investigated in unpoled soft lead zirconate titanate (PZT) ceramic where the texture symmetry m∞∞ forbids macropiezoelectricity. Even under high strain gradient (1 m−1) the induced polarization is small (1.6 μC/m2) at 20 °C. Higher strain gradients induce ferroelastic poling and an additional extrinsic contribution to the flexoelectric coefficient μ12 raising the value from 0.5 to 2.0 μC/m. Cooling through the Curie point (TC) under maximum stress (80 MPa) where the peak permittivity (∼20 000) could raise μ12 to 20 μC/m, the equivalent electric field is still only ∼1 kV/m, inadequate to achieve significant ferroelectric poling. The situation may be different in thin PZT films where much larger strain gradients can occur.</abstract><doi>10.1063/1.1570517</doi><tpages>3</tpages></addata></record> |
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title | Strain-gradient-induced electric polarization in lead zirconate titanate ceramics |
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