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dc.contributor.authorJunaidah, Osman
dc.contributor.authorTilley, David Reginald
dc.contributor.authorRosy, Teh
dc.contributor.authorIshibashi, Y.
dc.contributor.authorMohamad Nazri, Abdul Halif
dc.contributor.authorKhian, Hooi Chew
dc.date.accessioned2009-07-29T08:37:41Z
dc.date.available2009-07-29T08:37:41Z
dc.date.issued2006
dc.identifier.citationEuropean Physical Journal B, vol. 52 (1), July 2006, pages 143-150en_US
dc.identifier.issn1434-6028 (Print)
dc.identifier.issn1434-6036 (Online)
dc.identifier.urihttp://www.springerlink.com/content/l10041r882v77054/
dc.identifier.urihttp://dspace.unimap.edu.my/123456789/6614
dc.descriptionLink to publisher's homepage at http://www.springerlink.comen_US
dc.description.abstractIn the presence of a surface the Landau-Devonshire equations of ferroelectricity must be extended to include a boundary condition. For a ferroelectric with a second-order transition in the case when the polarization p(z) increases at the surface, it is well known that a surface state occurs in a range of temperature above the bulk critical temperature tCB . Here we explore the corresponding effect for a first-order ferroelectric. We show that a surface state can occur, but only if the surface effect is sufficiently strong. Analytic expressions are derived and illustrated for p(z), the surface value pS =p(0) and the free energy. The transition from the paraelectric state (p=0) to the surface state is first order, and for completeness we establish the dependence of the three critical temperatures (supercooling, thermodynamic and superheating) on a boundary-condition parameter y. In a final section, we derive and illustrate expressions for p(z)in the temperature range t<tCB.en_US
dc.language.isoenen_US
dc.publisherSpringer Berlin / Heidelbergen_US
dc.subjectFerroelectricityen_US
dc.subjectPolarization (Electricity)en_US
dc.subjectFerroelectricityen_US
dc.subjectLandau theoryen_US
dc.titleSurface state on first-order ferroelectricsen_US
dc.typeArticleen_US


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