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Mode Coupling at around M-Point in PZT
The question of the microscopic origin of the M-superstructure and additional satellite peaks in the Zr-rich lead zirconate-titanate is discussed for nearly 50 years. Clear contradiction between the selection rules of the critical scattering and the superstructure was found preventing unambiguous at...
Autores principales: | , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2021
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8746170/ https://www.ncbi.nlm.nih.gov/pubmed/35009227 http://dx.doi.org/10.3390/ma15010079 |
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author | Vakhrushev, Sergey Filimonov, Alexey Petroukhno, Konstantin Rudskoy, Andrey Udovenko, Stanislav Leontyev, Igor Bosak, Alexei |
author_facet | Vakhrushev, Sergey Filimonov, Alexey Petroukhno, Konstantin Rudskoy, Andrey Udovenko, Stanislav Leontyev, Igor Bosak, Alexei |
author_sort | Vakhrushev, Sergey |
collection | PubMed |
description | The question of the microscopic origin of the M-superstructure and additional satellite peaks in the Zr-rich lead zirconate-titanate is discussed for nearly 50 years. Clear contradiction between the selection rules of the critical scattering and the superstructure was found preventing unambiguous attributing of the observed superstructure either to the rotation of the oxygen octahedra or to the antiparallel displacements of the lead cations. Detailed analysis of the satellite pattern explained it as the result of the incommensurate phase transition rather than antiphase domains. Critical dynamics is the key point for the formulated problems. Recently, the oxygen tilt soft mode in the PbZr [Formula: see text] Ti [Formula: see text] O [Formula: see text] (PZT2.4) was found. But this does not resolve the extinction rules contradiction. The results of the inelastic X-ray scattering study of the phonon spectra of PZT2.4 around M-point are reported. Strong coupling between the lead and oxygen modes resulting in mode anticrossing and creation of the wide flat part in the lowest phonon dispersion curves is identified. This flat part corresponds to the mixture of the displacements of the lead and oxygen ions and can be an explanation of the extinction rules contradiction. Moreover, a flat dispersion surface is a typical prerequisite for the incommensurate phase transition. |
format | Online Article Text |
id | pubmed-8746170 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-87461702022-01-11 Mode Coupling at around M-Point in PZT Vakhrushev, Sergey Filimonov, Alexey Petroukhno, Konstantin Rudskoy, Andrey Udovenko, Stanislav Leontyev, Igor Bosak, Alexei Materials (Basel) Article The question of the microscopic origin of the M-superstructure and additional satellite peaks in the Zr-rich lead zirconate-titanate is discussed for nearly 50 years. Clear contradiction between the selection rules of the critical scattering and the superstructure was found preventing unambiguous attributing of the observed superstructure either to the rotation of the oxygen octahedra or to the antiparallel displacements of the lead cations. Detailed analysis of the satellite pattern explained it as the result of the incommensurate phase transition rather than antiphase domains. Critical dynamics is the key point for the formulated problems. Recently, the oxygen tilt soft mode in the PbZr [Formula: see text] Ti [Formula: see text] O [Formula: see text] (PZT2.4) was found. But this does not resolve the extinction rules contradiction. The results of the inelastic X-ray scattering study of the phonon spectra of PZT2.4 around M-point are reported. Strong coupling between the lead and oxygen modes resulting in mode anticrossing and creation of the wide flat part in the lowest phonon dispersion curves is identified. This flat part corresponds to the mixture of the displacements of the lead and oxygen ions and can be an explanation of the extinction rules contradiction. Moreover, a flat dispersion surface is a typical prerequisite for the incommensurate phase transition. MDPI 2021-12-23 /pmc/articles/PMC8746170/ /pubmed/35009227 http://dx.doi.org/10.3390/ma15010079 Text en © 2021 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Vakhrushev, Sergey Filimonov, Alexey Petroukhno, Konstantin Rudskoy, Andrey Udovenko, Stanislav Leontyev, Igor Bosak, Alexei Mode Coupling at around M-Point in PZT |
title | Mode Coupling at around M-Point in PZT |
title_full | Mode Coupling at around M-Point in PZT |
title_fullStr | Mode Coupling at around M-Point in PZT |
title_full_unstemmed | Mode Coupling at around M-Point in PZT |
title_short | Mode Coupling at around M-Point in PZT |
title_sort | mode coupling at around m-point in pzt |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8746170/ https://www.ncbi.nlm.nih.gov/pubmed/35009227 http://dx.doi.org/10.3390/ma15010079 |
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