Synthesis and dielectric properties of Pb 0.85 Ba 0.25 Zr 0.53 Ti 0.47 O 3 compounds with nano‐inclusions of Cu and Ni

Ceramic piezomaterials based on Pb 0.75 Ba 0.15 Zr 0.53 Ti 0.47 O 3 (PBZT) system are characterized by high values of the ferroelectric Curie temperature and polarization. They have widespread applications in electromechanical and electroacoustic transducers, bandwidth filters, transformers, frequen...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Physica status solidi. C 2013-04, Vol.10 (4), p.640-645
Hauptverfasser: Gurskii, L. I., Macutkevic, J., Banys, J., Poddubskaya, A., Saraseko, M. N., Petrov, A. V., Kalanda, N. A., Sobolev, N. A.
Format: Artikel
Sprache:eng
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 645
container_issue 4
container_start_page 640
container_title Physica status solidi. C
container_volume 10
creator Gurskii, L. I.
Macutkevic, J.
Banys, J.
Poddubskaya, A.
Saraseko, M. N.
Petrov, A. V.
Kalanda, N. A.
Sobolev, N. A.
description Ceramic piezomaterials based on Pb 0.75 Ba 0.15 Zr 0.53 Ti 0.47 O 3 (PBZT) system are characterized by high values of the ferroelectric Curie temperature and polarization. They have widespread applications in electromechanical and electroacoustic transducers, bandwidth filters, transformers, frequency stabilized resonators, etc. Preparation of PBZT composites with nano‐inclusions of Cu and Ni have been carried out by a complex powder technology including metallization procedures which were performed by the well‐known chemical deposition method from standard solutions of copper and nickel. Studies of hydrostatic density and porosity of obtained samples as well as their microstructural investigations have yielded a larger density of PBZT‐metal composites (5.3 – 7.3 g/cm 3 ) as compared with pure PBZT (4.7 g/cm 3 ). Measurements of dielectric properties of samples in the frequency range from 20 Hz – 1 MHz have shown that the Curie temperature increases in PBZT (Ni) and decreases in PBZT(Cu) in comparison with pure PBZT. The complex dielectric permittivity of all investigated composites at higher temperatures and low frequencies is mainly caused by the high electrical conductivity. Only at the highest frequency used (1 MHz) the real part of the complex permittivity is caused by a resonant soft mode and could be fitted with the Curie‐Weiss law. The activation energy of ferroelectric domain mobility in PBZT (Cu, Ni) composites is lower than in pure PBZT. This can be explained by a decrease of the domain size in composites. (© 2013 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)
doi_str_mv 10.1002/pssc.201200915
format Article
fullrecord <record><control><sourceid>crossref</sourceid><recordid>TN_cdi_crossref_primary_10_1002_pssc_201200915</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>10_1002_pssc_201200915</sourcerecordid><originalsourceid>FETCH-LOGICAL-c845-b3b11775e63fc1bb21e4402b607c0562720a3f7880376711a8f6cfdc2ca35ddd3</originalsourceid><addsrcrecordid>eNo9kEtOwzAURS0EEqUwZewNJLxnx3YYQsVPqigSHTGJHH9Uo9aJ7FTQGUtgjayEFBCjc0fnSoeQc4QSAdhFn7MpGSADuERxQCYoEQqUFTscdy1ZIbnAY3KS8ysAF4ByQt6fd3FYuRwy1dFSG9zamSEFQ_vU9S4NwWXaefrUUihrQa_1SCboSxopOF2GkZWiC8qp6TZ9t40207cwrGjUsfv6-AzRrLc5dPHHM9v-_DyGU3Lk9Tq7sz9OyfL2Zjm7L-aLu4fZ1bwwdSWKlreISgknuTfYtgxdVQFrJSgDQjLFQHOv6hq4kgpR114abw0zmgtrLZ-S8ldrUpdzcr7pU9jotGsQmn22Zp-t-c_GvwHfBV5S</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Synthesis and dielectric properties of Pb 0.85 Ba 0.25 Zr 0.53 Ti 0.47 O 3 compounds with nano‐inclusions of Cu and Ni</title><source>Wiley Journals</source><creator>Gurskii, L. I. ; Macutkevic, J. ; Banys, J. ; Poddubskaya, A. ; Saraseko, M. N. ; Petrov, A. V. ; Kalanda, N. A. ; Sobolev, N. A.</creator><creatorcontrib>Gurskii, L. I. ; Macutkevic, J. ; Banys, J. ; Poddubskaya, A. ; Saraseko, M. N. ; Petrov, A. V. ; Kalanda, N. A. ; Sobolev, N. A.</creatorcontrib><description>Ceramic piezomaterials based on Pb 0.75 Ba 0.15 Zr 0.53 Ti 0.47 O 3 (PBZT) system are characterized by high values of the ferroelectric Curie temperature and polarization. They have widespread applications in electromechanical and electroacoustic transducers, bandwidth filters, transformers, frequency stabilized resonators, etc. Preparation of PBZT composites with nano‐inclusions of Cu and Ni have been carried out by a complex powder technology including metallization procedures which were performed by the well‐known chemical deposition method from standard solutions of copper and nickel. Studies of hydrostatic density and porosity of obtained samples as well as their microstructural investigations have yielded a larger density of PBZT‐metal composites (5.3 – 7.3 g/cm 3 ) as compared with pure PBZT (4.7 g/cm 3 ). Measurements of dielectric properties of samples in the frequency range from 20 Hz – 1 MHz have shown that the Curie temperature increases in PBZT (Ni) and decreases in PBZT(Cu) in comparison with pure PBZT. The complex dielectric permittivity of all investigated composites at higher temperatures and low frequencies is mainly caused by the high electrical conductivity. Only at the highest frequency used (1 MHz) the real part of the complex permittivity is caused by a resonant soft mode and could be fitted with the Curie‐Weiss law. The activation energy of ferroelectric domain mobility in PBZT (Cu, Ni) composites is lower than in pure PBZT. This can be explained by a decrease of the domain size in composites. (© 2013 WILEY‐VCH Verlag GmbH &amp; Co. KGaA, Weinheim)</description><identifier>ISSN: 1862-6351</identifier><identifier>EISSN: 1610-1642</identifier><identifier>DOI: 10.1002/pssc.201200915</identifier><language>eng</language><ispartof>Physica status solidi. C, 2013-04, Vol.10 (4), p.640-645</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c845-b3b11775e63fc1bb21e4402b607c0562720a3f7880376711a8f6cfdc2ca35ddd3</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Gurskii, L. I.</creatorcontrib><creatorcontrib>Macutkevic, J.</creatorcontrib><creatorcontrib>Banys, J.</creatorcontrib><creatorcontrib>Poddubskaya, A.</creatorcontrib><creatorcontrib>Saraseko, M. N.</creatorcontrib><creatorcontrib>Petrov, A. V.</creatorcontrib><creatorcontrib>Kalanda, N. A.</creatorcontrib><creatorcontrib>Sobolev, N. A.</creatorcontrib><title>Synthesis and dielectric properties of Pb 0.85 Ba 0.25 Zr 0.53 Ti 0.47 O 3 compounds with nano‐inclusions of Cu and Ni</title><title>Physica status solidi. C</title><description>Ceramic piezomaterials based on Pb 0.75 Ba 0.15 Zr 0.53 Ti 0.47 O 3 (PBZT) system are characterized by high values of the ferroelectric Curie temperature and polarization. They have widespread applications in electromechanical and electroacoustic transducers, bandwidth filters, transformers, frequency stabilized resonators, etc. Preparation of PBZT composites with nano‐inclusions of Cu and Ni have been carried out by a complex powder technology including metallization procedures which were performed by the well‐known chemical deposition method from standard solutions of copper and nickel. Studies of hydrostatic density and porosity of obtained samples as well as their microstructural investigations have yielded a larger density of PBZT‐metal composites (5.3 – 7.3 g/cm 3 ) as compared with pure PBZT (4.7 g/cm 3 ). Measurements of dielectric properties of samples in the frequency range from 20 Hz – 1 MHz have shown that the Curie temperature increases in PBZT (Ni) and decreases in PBZT(Cu) in comparison with pure PBZT. The complex dielectric permittivity of all investigated composites at higher temperatures and low frequencies is mainly caused by the high electrical conductivity. Only at the highest frequency used (1 MHz) the real part of the complex permittivity is caused by a resonant soft mode and could be fitted with the Curie‐Weiss law. The activation energy of ferroelectric domain mobility in PBZT (Cu, Ni) composites is lower than in pure PBZT. This can be explained by a decrease of the domain size in composites. (© 2013 WILEY‐VCH Verlag GmbH &amp; Co. KGaA, Weinheim)</description><issn>1862-6351</issn><issn>1610-1642</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNo9kEtOwzAURS0EEqUwZewNJLxnx3YYQsVPqigSHTGJHH9Uo9aJ7FTQGUtgjayEFBCjc0fnSoeQc4QSAdhFn7MpGSADuERxQCYoEQqUFTscdy1ZIbnAY3KS8ysAF4ByQt6fd3FYuRwy1dFSG9zamSEFQ_vU9S4NwWXaefrUUihrQa_1SCboSxopOF2GkZWiC8qp6TZ9t40207cwrGjUsfv6-AzRrLc5dPHHM9v-_DyGU3Lk9Tq7sz9OyfL2Zjm7L-aLu4fZ1bwwdSWKlreISgknuTfYtgxdVQFrJSgDQjLFQHOv6hq4kgpR114abw0zmgtrLZ-S8ldrUpdzcr7pU9jotGsQmn22Zp-t-c_GvwHfBV5S</recordid><startdate>201304</startdate><enddate>201304</enddate><creator>Gurskii, L. I.</creator><creator>Macutkevic, J.</creator><creator>Banys, J.</creator><creator>Poddubskaya, A.</creator><creator>Saraseko, M. N.</creator><creator>Petrov, A. V.</creator><creator>Kalanda, N. A.</creator><creator>Sobolev, N. A.</creator><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>201304</creationdate><title>Synthesis and dielectric properties of Pb 0.85 Ba 0.25 Zr 0.53 Ti 0.47 O 3 compounds with nano‐inclusions of Cu and Ni</title><author>Gurskii, L. I. ; Macutkevic, J. ; Banys, J. ; Poddubskaya, A. ; Saraseko, M. N. ; Petrov, A. V. ; Kalanda, N. A. ; Sobolev, N. A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c845-b3b11775e63fc1bb21e4402b607c0562720a3f7880376711a8f6cfdc2ca35ddd3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Gurskii, L. I.</creatorcontrib><creatorcontrib>Macutkevic, J.</creatorcontrib><creatorcontrib>Banys, J.</creatorcontrib><creatorcontrib>Poddubskaya, A.</creatorcontrib><creatorcontrib>Saraseko, M. N.</creatorcontrib><creatorcontrib>Petrov, A. V.</creatorcontrib><creatorcontrib>Kalanda, N. A.</creatorcontrib><creatorcontrib>Sobolev, N. A.</creatorcontrib><collection>CrossRef</collection><jtitle>Physica status solidi. C</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Gurskii, L. I.</au><au>Macutkevic, J.</au><au>Banys, J.</au><au>Poddubskaya, A.</au><au>Saraseko, M. N.</au><au>Petrov, A. V.</au><au>Kalanda, N. A.</au><au>Sobolev, N. A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Synthesis and dielectric properties of Pb 0.85 Ba 0.25 Zr 0.53 Ti 0.47 O 3 compounds with nano‐inclusions of Cu and Ni</atitle><jtitle>Physica status solidi. C</jtitle><date>2013-04</date><risdate>2013</risdate><volume>10</volume><issue>4</issue><spage>640</spage><epage>645</epage><pages>640-645</pages><issn>1862-6351</issn><eissn>1610-1642</eissn><abstract>Ceramic piezomaterials based on Pb 0.75 Ba 0.15 Zr 0.53 Ti 0.47 O 3 (PBZT) system are characterized by high values of the ferroelectric Curie temperature and polarization. They have widespread applications in electromechanical and electroacoustic transducers, bandwidth filters, transformers, frequency stabilized resonators, etc. Preparation of PBZT composites with nano‐inclusions of Cu and Ni have been carried out by a complex powder technology including metallization procedures which were performed by the well‐known chemical deposition method from standard solutions of copper and nickel. Studies of hydrostatic density and porosity of obtained samples as well as their microstructural investigations have yielded a larger density of PBZT‐metal composites (5.3 – 7.3 g/cm 3 ) as compared with pure PBZT (4.7 g/cm 3 ). Measurements of dielectric properties of samples in the frequency range from 20 Hz – 1 MHz have shown that the Curie temperature increases in PBZT (Ni) and decreases in PBZT(Cu) in comparison with pure PBZT. The complex dielectric permittivity of all investigated composites at higher temperatures and low frequencies is mainly caused by the high electrical conductivity. Only at the highest frequency used (1 MHz) the real part of the complex permittivity is caused by a resonant soft mode and could be fitted with the Curie‐Weiss law. The activation energy of ferroelectric domain mobility in PBZT (Cu, Ni) composites is lower than in pure PBZT. This can be explained by a decrease of the domain size in composites. (© 2013 WILEY‐VCH Verlag GmbH &amp; Co. KGaA, Weinheim)</abstract><doi>10.1002/pssc.201200915</doi><tpages>6</tpages></addata></record>
fulltext fulltext
identifier ISSN: 1862-6351
ispartof Physica status solidi. C, 2013-04, Vol.10 (4), p.640-645
issn 1862-6351
1610-1642
language eng
recordid cdi_crossref_primary_10_1002_pssc_201200915
source Wiley Journals
title Synthesis and dielectric properties of Pb 0.85 Ba 0.25 Zr 0.53 Ti 0.47 O 3 compounds with nano‐inclusions of Cu and Ni
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-25T22%3A49%3A36IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-crossref&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Synthesis%20and%20dielectric%20properties%20of%20Pb%200.85%20Ba%200.25%20Zr%200.53%20Ti%200.47%20O%203%20compounds%20with%20nano%E2%80%90inclusions%20of%20Cu%20and%20Ni&rft.jtitle=Physica%20status%20solidi.%20C&rft.au=Gurskii,%20L.%20I.&rft.date=2013-04&rft.volume=10&rft.issue=4&rft.spage=640&rft.epage=645&rft.pages=640-645&rft.issn=1862-6351&rft.eissn=1610-1642&rft_id=info:doi/10.1002/pssc.201200915&rft_dat=%3Ccrossref%3E10_1002_pssc_201200915%3C/crossref%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true