Enhanced polarization by the coherent heterophase interface between polar and non-polar phases
A piezoelectric composite containing the ferroelectric polar (Bi(Na 0.8 K 0.2 ) 0.5 TiO 3 : f-BNKT) and the non-polar (0.94Bi(Na 0.75 K 0.25 ) 0.5 TiO 3 -0.06BiAlO 3 : BNKT-BA) phases exhibits synergetic properties which combine the beneficial aspects of each phase, i.e. , the high saturated polariz...
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creator | Kim, Gi-Yeop Sung, Kil-Dong Rhyim, Youngmok Yoon, Seog-Young Kim, Min-Soo Jeong, Soon-Jong Kim, Kwang-Ho Ryu, Jungho Kim, Sung-Dae Choi, Si-Young |
description | A piezoelectric composite containing the ferroelectric polar (Bi(Na
0.8
K
0.2
)
0.5
TiO
3
: f-BNKT) and the non-polar (0.94Bi(Na
0.75
K
0.25
)
0.5
TiO
3
-0.06BiAlO
3
: BNKT-BA) phases exhibits synergetic properties which combine the beneficial aspects of each phase,
i.e.
, the high saturated polarization (
P
s
) of the polar phase and the low coercive field (
E
c
) of the non-polar phase. To understand the origin of such a fruitful outcome from this type of polar/non-polar heterophase structure, comprehensive studies are conducted, including transmission electron microscopy (TEM) and finite element method (FEM) analyses. The TEM results show that the polar/non-polar composite has a core/shell structure in which the polar phase (core) is surrounded by a non-polar phase (shell).
In situ
electrical biasing TEM experiments visualize that the ferroelectric domains in the polar core are aligned even under an electric field of ∼1 kV mm
−1
, which is much lower than its intrinsic coercive field (∼3 kV mm
−1
). From the FEM analyses, we can find that the enhanced polarization of the polar phase is promoted by an additional internal field at the phase boundary which originates from the preferential polarization of the relaxor-like non-polar phase. From the present study, we conclude that the coherent interface between polar and non-polar phases is a key factor for understanding the enhanced piezoelectric properties of the composite.
The electric polarization behavior of a Bi-based piezoelectric ceramic is tuned by building a polar (core)/non-polar (shell) heterostructure. |
doi_str_mv | 10.1039/c5nr05391a |
format | Article |
fullrecord | <record><control><sourceid>proquest_pubme</sourceid><recordid>TN_cdi_pubmed_primary_26601654</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>1777987583</sourcerecordid><originalsourceid>FETCH-LOGICAL-c408t-3d6db4ec743993e04416c19098adb932edf8ac784b59d696cc7132d7b5917f063</originalsourceid><addsrcrecordid>eNqFkUtPwzAQhC0EoqVw4Q7yESEF7Njx41hV5SEhkBBciRx7owSlTrFTofLrCU0pR047o_12DrMInVJyRQnT1zbzgWRMU7OHxinhJGFMpvs7LfgIHcX4TojQTLBDNEqFIFRkfIze5r4y3oLDy7Yxof4yXd16XKxxVwG2bQUBfIcr6CC0y8pEwLXvdWks4AK6TwA_nGLjHfatTwa3YeMxOihNE-FkOyfo9Wb-MrtLHp5u72fTh8RyorqEOeEKDlZypjUDwjkVlmqilXGFZim4UhkrFS8y7YQW1krKUid7S2VJBJugiyF3GdqPFcQuX9TRQtMYD-0q5lQRRYmWGf0flVJqJTPFevRyQG1oYwxQ5stQL0xY55TkP9Xns-zxeVP9tIfPt7mrYgFuh_523QNnAxCi3W3_fse-AXYtiKg</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>1777987583</pqid></control><display><type>article</type><title>Enhanced polarization by the coherent heterophase interface between polar and non-polar phases</title><source>Royal Society Of Chemistry Journals 2008-</source><source>Alma/SFX Local Collection</source><creator>Kim, Gi-Yeop ; Sung, Kil-Dong ; Rhyim, Youngmok ; Yoon, Seog-Young ; Kim, Min-Soo ; Jeong, Soon-Jong ; Kim, Kwang-Ho ; Ryu, Jungho ; Kim, Sung-Dae ; Choi, Si-Young</creator><creatorcontrib>Kim, Gi-Yeop ; Sung, Kil-Dong ; Rhyim, Youngmok ; Yoon, Seog-Young ; Kim, Min-Soo ; Jeong, Soon-Jong ; Kim, Kwang-Ho ; Ryu, Jungho ; Kim, Sung-Dae ; Choi, Si-Young</creatorcontrib><description>A piezoelectric composite containing the ferroelectric polar (Bi(Na
0.8
K
0.2
)
0.5
TiO
3
: f-BNKT) and the non-polar (0.94Bi(Na
0.75
K
0.25
)
0.5
TiO
3
-0.06BiAlO
3
: BNKT-BA) phases exhibits synergetic properties which combine the beneficial aspects of each phase,
i.e.
, the high saturated polarization (
P
s
) of the polar phase and the low coercive field (
E
c
) of the non-polar phase. To understand the origin of such a fruitful outcome from this type of polar/non-polar heterophase structure, comprehensive studies are conducted, including transmission electron microscopy (TEM) and finite element method (FEM) analyses. The TEM results show that the polar/non-polar composite has a core/shell structure in which the polar phase (core) is surrounded by a non-polar phase (shell).
In situ
electrical biasing TEM experiments visualize that the ferroelectric domains in the polar core are aligned even under an electric field of ∼1 kV mm
−1
, which is much lower than its intrinsic coercive field (∼3 kV mm
−1
). From the FEM analyses, we can find that the enhanced polarization of the polar phase is promoted by an additional internal field at the phase boundary which originates from the preferential polarization of the relaxor-like non-polar phase. From the present study, we conclude that the coherent interface between polar and non-polar phases is a key factor for understanding the enhanced piezoelectric properties of the composite.
The electric polarization behavior of a Bi-based piezoelectric ceramic is tuned by building a polar (core)/non-polar (shell) heterostructure.</description><identifier>ISSN: 2040-3364</identifier><identifier>EISSN: 2040-3372</identifier><identifier>DOI: 10.1039/c5nr05391a</identifier><identifier>PMID: 26601654</identifier><language>eng</language><publisher>England</publisher><subject>Coercive force ; Coherence ; Finite element method ; Mathematical models ; Phases ; Piezoelectricity ; Polarization ; Transmission electron microscopy</subject><ispartof>Nanoscale, 2016-04, Vol.8 (14), p.7443-7448</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c408t-3d6db4ec743993e04416c19098adb932edf8ac784b59d696cc7132d7b5917f063</citedby><cites>FETCH-LOGICAL-c408t-3d6db4ec743993e04416c19098adb932edf8ac784b59d696cc7132d7b5917f063</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/26601654$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Kim, Gi-Yeop</creatorcontrib><creatorcontrib>Sung, Kil-Dong</creatorcontrib><creatorcontrib>Rhyim, Youngmok</creatorcontrib><creatorcontrib>Yoon, Seog-Young</creatorcontrib><creatorcontrib>Kim, Min-Soo</creatorcontrib><creatorcontrib>Jeong, Soon-Jong</creatorcontrib><creatorcontrib>Kim, Kwang-Ho</creatorcontrib><creatorcontrib>Ryu, Jungho</creatorcontrib><creatorcontrib>Kim, Sung-Dae</creatorcontrib><creatorcontrib>Choi, Si-Young</creatorcontrib><title>Enhanced polarization by the coherent heterophase interface between polar and non-polar phases</title><title>Nanoscale</title><addtitle>Nanoscale</addtitle><description>A piezoelectric composite containing the ferroelectric polar (Bi(Na
0.8
K
0.2
)
0.5
TiO
3
: f-BNKT) and the non-polar (0.94Bi(Na
0.75
K
0.25
)
0.5
TiO
3
-0.06BiAlO
3
: BNKT-BA) phases exhibits synergetic properties which combine the beneficial aspects of each phase,
i.e.
, the high saturated polarization (
P
s
) of the polar phase and the low coercive field (
E
c
) of the non-polar phase. To understand the origin of such a fruitful outcome from this type of polar/non-polar heterophase structure, comprehensive studies are conducted, including transmission electron microscopy (TEM) and finite element method (FEM) analyses. The TEM results show that the polar/non-polar composite has a core/shell structure in which the polar phase (core) is surrounded by a non-polar phase (shell).
In situ
electrical biasing TEM experiments visualize that the ferroelectric domains in the polar core are aligned even under an electric field of ∼1 kV mm
−1
, which is much lower than its intrinsic coercive field (∼3 kV mm
−1
). From the FEM analyses, we can find that the enhanced polarization of the polar phase is promoted by an additional internal field at the phase boundary which originates from the preferential polarization of the relaxor-like non-polar phase. From the present study, we conclude that the coherent interface between polar and non-polar phases is a key factor for understanding the enhanced piezoelectric properties of the composite.
The electric polarization behavior of a Bi-based piezoelectric ceramic is tuned by building a polar (core)/non-polar (shell) heterostructure.</description><subject>Coercive force</subject><subject>Coherence</subject><subject>Finite element method</subject><subject>Mathematical models</subject><subject>Phases</subject><subject>Piezoelectricity</subject><subject>Polarization</subject><subject>Transmission electron microscopy</subject><issn>2040-3364</issn><issn>2040-3372</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNqFkUtPwzAQhC0EoqVw4Q7yESEF7Njx41hV5SEhkBBciRx7owSlTrFTofLrCU0pR047o_12DrMInVJyRQnT1zbzgWRMU7OHxinhJGFMpvs7LfgIHcX4TojQTLBDNEqFIFRkfIze5r4y3oLDy7Yxof4yXd16XKxxVwG2bQUBfIcr6CC0y8pEwLXvdWks4AK6TwA_nGLjHfatTwa3YeMxOihNE-FkOyfo9Wb-MrtLHp5u72fTh8RyorqEOeEKDlZypjUDwjkVlmqilXGFZim4UhkrFS8y7YQW1krKUid7S2VJBJugiyF3GdqPFcQuX9TRQtMYD-0q5lQRRYmWGf0flVJqJTPFevRyQG1oYwxQ5stQL0xY55TkP9Xns-zxeVP9tIfPt7mrYgFuh_523QNnAxCi3W3_fse-AXYtiKg</recordid><startdate>20160414</startdate><enddate>20160414</enddate><creator>Kim, Gi-Yeop</creator><creator>Sung, Kil-Dong</creator><creator>Rhyim, Youngmok</creator><creator>Yoon, Seog-Young</creator><creator>Kim, Min-Soo</creator><creator>Jeong, Soon-Jong</creator><creator>Kim, Kwang-Ho</creator><creator>Ryu, Jungho</creator><creator>Kim, Sung-Dae</creator><creator>Choi, Si-Young</creator><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>7SR</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>F28</scope><scope>FR3</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20160414</creationdate><title>Enhanced polarization by the coherent heterophase interface between polar and non-polar phases</title><author>Kim, Gi-Yeop ; Sung, Kil-Dong ; Rhyim, Youngmok ; Yoon, Seog-Young ; Kim, Min-Soo ; Jeong, Soon-Jong ; Kim, Kwang-Ho ; Ryu, Jungho ; Kim, Sung-Dae ; Choi, Si-Young</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c408t-3d6db4ec743993e04416c19098adb932edf8ac784b59d696cc7132d7b5917f063</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Coercive force</topic><topic>Coherence</topic><topic>Finite element method</topic><topic>Mathematical models</topic><topic>Phases</topic><topic>Piezoelectricity</topic><topic>Polarization</topic><topic>Transmission electron microscopy</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kim, Gi-Yeop</creatorcontrib><creatorcontrib>Sung, Kil-Dong</creatorcontrib><creatorcontrib>Rhyim, Youngmok</creatorcontrib><creatorcontrib>Yoon, Seog-Young</creatorcontrib><creatorcontrib>Kim, Min-Soo</creatorcontrib><creatorcontrib>Jeong, Soon-Jong</creatorcontrib><creatorcontrib>Kim, Kwang-Ho</creatorcontrib><creatorcontrib>Ryu, Jungho</creatorcontrib><creatorcontrib>Kim, Sung-Dae</creatorcontrib><creatorcontrib>Choi, Si-Young</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>Engineered Materials Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>ANTE: Abstracts in New Technology & Engineering</collection><collection>Engineering Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Nanoscale</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kim, Gi-Yeop</au><au>Sung, Kil-Dong</au><au>Rhyim, Youngmok</au><au>Yoon, Seog-Young</au><au>Kim, Min-Soo</au><au>Jeong, Soon-Jong</au><au>Kim, Kwang-Ho</au><au>Ryu, Jungho</au><au>Kim, Sung-Dae</au><au>Choi, Si-Young</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Enhanced polarization by the coherent heterophase interface between polar and non-polar phases</atitle><jtitle>Nanoscale</jtitle><addtitle>Nanoscale</addtitle><date>2016-04-14</date><risdate>2016</risdate><volume>8</volume><issue>14</issue><spage>7443</spage><epage>7448</epage><pages>7443-7448</pages><issn>2040-3364</issn><eissn>2040-3372</eissn><abstract>A piezoelectric composite containing the ferroelectric polar (Bi(Na
0.8
K
0.2
)
0.5
TiO
3
: f-BNKT) and the non-polar (0.94Bi(Na
0.75
K
0.25
)
0.5
TiO
3
-0.06BiAlO
3
: BNKT-BA) phases exhibits synergetic properties which combine the beneficial aspects of each phase,
i.e.
, the high saturated polarization (
P
s
) of the polar phase and the low coercive field (
E
c
) of the non-polar phase. To understand the origin of such a fruitful outcome from this type of polar/non-polar heterophase structure, comprehensive studies are conducted, including transmission electron microscopy (TEM) and finite element method (FEM) analyses. The TEM results show that the polar/non-polar composite has a core/shell structure in which the polar phase (core) is surrounded by a non-polar phase (shell).
In situ
electrical biasing TEM experiments visualize that the ferroelectric domains in the polar core are aligned even under an electric field of ∼1 kV mm
−1
, which is much lower than its intrinsic coercive field (∼3 kV mm
−1
). From the FEM analyses, we can find that the enhanced polarization of the polar phase is promoted by an additional internal field at the phase boundary which originates from the preferential polarization of the relaxor-like non-polar phase. From the present study, we conclude that the coherent interface between polar and non-polar phases is a key factor for understanding the enhanced piezoelectric properties of the composite.
The electric polarization behavior of a Bi-based piezoelectric ceramic is tuned by building a polar (core)/non-polar (shell) heterostructure.</abstract><cop>England</cop><pmid>26601654</pmid><doi>10.1039/c5nr05391a</doi><tpages>6</tpages></addata></record> |
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source | Royal Society Of Chemistry Journals 2008-; Alma/SFX Local Collection |
subjects | Coercive force Coherence Finite element method Mathematical models Phases Piezoelectricity Polarization Transmission electron microscopy |
title | Enhanced polarization by the coherent heterophase interface between polar and non-polar phases |
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