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Response of the electric field gradient in ion implanted BaTiO$_{3}$ to an external electric field
Single crystalline, ferroelectric BaTiO$_{3}$ as material with the highest piezoelectric constants among the perovskites with ordered sublattices was implanted with $^{111}$In($^{111}$Cd). The electric field gradient at the Ti position was measured with perturbed $\gamma-\gamma$-angular correlation...
Autores principales: | , , , , , |
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Lenguaje: | eng |
Publicado: |
2000
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1557/PROC-655-CC10.11.1 http://cds.cern.ch/record/524750 |
_version_ | 1780897876858109952 |
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author | Dietrich, M Bartels, Julius Deicher, M Freitag, K Samokhvalov, V Unterricker, S |
author_facet | Dietrich, M Bartels, Julius Deicher, M Freitag, K Samokhvalov, V Unterricker, S |
author_sort | Dietrich, M |
collection | CERN |
description | Single crystalline, ferroelectric BaTiO$_{3}$ as material with the highest piezoelectric constants among the perovskites with ordered sublattices was implanted with $^{111}$In($^{111}$Cd). The electric field gradient at the Ti position was measured with perturbed $\gamma-\gamma$-angular correlation spectroscopy (PAC) while the crystal was exposed to an external electric field. A quadratic dependence could be observed: $\nu_{Q}$(E) = (34.8(1) + 0.16(4) E/kV/mm + 0.080(2) E$^{2}$/kV$^{2}$/mm$^{2}$) MHz. Point charge model calculations reproduce the linear change of Vzz, but not the quadratic term. The polarizability of the host ions of BaTiO$_{3}$ is known to be nonlinear with respect to an electric field. The resulting quadratic shift of the electron density is reflected in the strength of the EFG. |
id | cern-524750 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2000 |
record_format | invenio |
spelling | cern-5247502019-09-30T06:29:59Zdoi:10.1557/PROC-655-CC10.11.1http://cds.cern.ch/record/524750engDietrich, MBartels, JuliusDeicher, MFreitag, KSamokhvalov, VUnterricker, SResponse of the electric field gradient in ion implanted BaTiO$_{3}$ to an external electric fieldCondensed MatterSingle crystalline, ferroelectric BaTiO$_{3}$ as material with the highest piezoelectric constants among the perovskites with ordered sublattices was implanted with $^{111}$In($^{111}$Cd). The electric field gradient at the Ti position was measured with perturbed $\gamma-\gamma$-angular correlation spectroscopy (PAC) while the crystal was exposed to an external electric field. A quadratic dependence could be observed: $\nu_{Q}$(E) = (34.8(1) + 0.16(4) E/kV/mm + 0.080(2) E$^{2}$/kV$^{2}$/mm$^{2}$) MHz. Point charge model calculations reproduce the linear change of Vzz, but not the quadratic term. The polarizability of the host ions of BaTiO$_{3}$ is known to be nonlinear with respect to an electric field. The resulting quadratic shift of the electron density is reflected in the strength of the EFG.CERN-OPEN-2001-072oai:cds.cern.ch:5247502000-12-22 |
spellingShingle | Condensed Matter Dietrich, M Bartels, Julius Deicher, M Freitag, K Samokhvalov, V Unterricker, S Response of the electric field gradient in ion implanted BaTiO$_{3}$ to an external electric field |
title | Response of the electric field gradient in ion implanted BaTiO$_{3}$ to an external electric field |
title_full | Response of the electric field gradient in ion implanted BaTiO$_{3}$ to an external electric field |
title_fullStr | Response of the electric field gradient in ion implanted BaTiO$_{3}$ to an external electric field |
title_full_unstemmed | Response of the electric field gradient in ion implanted BaTiO$_{3}$ to an external electric field |
title_short | Response of the electric field gradient in ion implanted BaTiO$_{3}$ to an external electric field |
title_sort | response of the electric field gradient in ion implanted batio$_{3}$ to an external electric field |
topic | Condensed Matter |
url | https://dx.doi.org/10.1557/PROC-655-CC10.11.1 http://cds.cern.ch/record/524750 |
work_keys_str_mv | AT dietrichm responseoftheelectricfieldgradientinionimplantedbatio3toanexternalelectricfield AT bartelsjulius responseoftheelectricfieldgradientinionimplantedbatio3toanexternalelectricfield AT deicherm responseoftheelectricfieldgradientinionimplantedbatio3toanexternalelectricfield AT freitagk responseoftheelectricfieldgradientinionimplantedbatio3toanexternalelectricfield AT samokhvalovv responseoftheelectricfieldgradientinionimplantedbatio3toanexternalelectricfield AT unterrickers responseoftheelectricfieldgradientinionimplantedbatio3toanexternalelectricfield |