Effect of the (Ba + Sr)/Ti ratio on the microwave‐tunable properties of Ba 0.6 Sr 0.4 TiO 3 ceramics
The impact of the (Ba + Sr)/Ti (A/B) ratio on the microwave‐tunable characteristics of diffuse phase transition ( DPT ) ferroelectric Ba 0.6 Sr 0.4 TiO 3 (0.6‐ BST ) ceramics was investigated. The reduction in the lattice constant with increasing nonstoichiometry was attributed to introduced partial...
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Veröffentlicht in: | Journal of the American Ceramic Society 2017-03, Vol.100 (3), p.1037-1043 |
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creator | Teranishi, Takashi Kanemoto, Riku Hayashi, Hidetaka Kishimoto, Akira |
description | The impact of the (Ba + Sr)/Ti (A/B) ratio on the microwave‐tunable characteristics of diffuse phase transition (
DPT
) ferroelectric Ba
0.6
Sr
0.4
TiO
3
(0.6‐
BST
) ceramics was investigated. The reduction in the lattice constant with increasing nonstoichiometry was attributed to introduced partial Schottky defects, i.e.,
and
. The magnitude of the dielectric constant, ε′, at room temperature in the absence of an applied electric field was governed by the shift in the dielectric maximum temperature,
T
m
, because
T
m
was close to room temperature for the 0.6‐
BST
. The dielectric loss, tanδ, diminished as the ε′ decreased for 0.98≤A/B≤1.05, while the tanδ was much higher for A/B=0.95 having the greatest A‐site vacancy loading. The negatively charged
and
were mainly compensated by oxygen vacancies and likely partly compensated by holes, h
•
, which contributed to the electrical conduction. The tunability,
T
, at 100 MHz was almost constant at 20%–25% for A/B≥1.00 despite the reduction of the ε′, whereas
T
decreased for A/B |
doi_str_mv | 10.1111/jace.14700 |
format | Article |
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DPT
) ferroelectric Ba
0.6
Sr
0.4
TiO
3
(0.6‐
BST
) ceramics was investigated. The reduction in the lattice constant with increasing nonstoichiometry was attributed to introduced partial Schottky defects, i.e.,
and
. The magnitude of the dielectric constant, ε′, at room temperature in the absence of an applied electric field was governed by the shift in the dielectric maximum temperature,
T
m
, because
T
m
was close to room temperature for the 0.6‐
BST
. The dielectric loss, tanδ, diminished as the ε′ decreased for 0.98≤A/B≤1.05, while the tanδ was much higher for A/B=0.95 having the greatest A‐site vacancy loading. The negatively charged
and
were mainly compensated by oxygen vacancies and likely partly compensated by holes, h
•
, which contributed to the electrical conduction. The tunability,
T
, at 100 MHz was almost constant at 20%–25% for A/B≥1.00 despite the reduction of the ε′, whereas
T
decreased for A/B<1.00 to
ca
. 10% for A/B=0.95 having the greatest A‐site vacancy loading. The results implied that the
for larger A/B values was more efficient in generating nucleation sites in the polar nanoregions (
PNR
s) than the
for smaller A/B values, thereby providing greater dipole polarization. Consequently, the figure of merit,
FOM
, reached its maximum of 250 at A/B=0.9875, which was
ca
. 155% higher than that of the stoichiometric
BST
.</description><identifier>ISSN: 0002-7820</identifier><identifier>EISSN: 1551-2916</identifier><identifier>DOI: 10.1111/jace.14700</identifier><language>eng</language><ispartof>Journal of the American Ceramic Society, 2017-03, Vol.100 (3), p.1037-1043</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c760-720afc1018b4ce9fc9aaa3fbbfe827de3530d42b61444533254299e05dcdce9b3</citedby><cites>FETCH-LOGICAL-c760-720afc1018b4ce9fc9aaa3fbbfe827de3530d42b61444533254299e05dcdce9b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,777,781,27905,27906</link.rule.ids></links><search><creatorcontrib>Teranishi, Takashi</creatorcontrib><creatorcontrib>Kanemoto, Riku</creatorcontrib><creatorcontrib>Hayashi, Hidetaka</creatorcontrib><creatorcontrib>Kishimoto, Akira</creatorcontrib><title>Effect of the (Ba + Sr)/Ti ratio on the microwave‐tunable properties of Ba 0.6 Sr 0.4 TiO 3 ceramics</title><title>Journal of the American Ceramic Society</title><description>The impact of the (Ba + Sr)/Ti (A/B) ratio on the microwave‐tunable characteristics of diffuse phase transition (
DPT
) ferroelectric Ba
0.6
Sr
0.4
TiO
3
(0.6‐
BST
) ceramics was investigated. The reduction in the lattice constant with increasing nonstoichiometry was attributed to introduced partial Schottky defects, i.e.,
and
. The magnitude of the dielectric constant, ε′, at room temperature in the absence of an applied electric field was governed by the shift in the dielectric maximum temperature,
T
m
, because
T
m
was close to room temperature for the 0.6‐
BST
. The dielectric loss, tanδ, diminished as the ε′ decreased for 0.98≤A/B≤1.05, while the tanδ was much higher for A/B=0.95 having the greatest A‐site vacancy loading. The negatively charged
and
were mainly compensated by oxygen vacancies and likely partly compensated by holes, h
•
, which contributed to the electrical conduction. The tunability,
T
, at 100 MHz was almost constant at 20%–25% for A/B≥1.00 despite the reduction of the ε′, whereas
T
decreased for A/B<1.00 to
ca
. 10% for A/B=0.95 having the greatest A‐site vacancy loading. The results implied that the
for larger A/B values was more efficient in generating nucleation sites in the polar nanoregions (
PNR
s) than the
for smaller A/B values, thereby providing greater dipole polarization. Consequently, the figure of merit,
FOM
, reached its maximum of 250 at A/B=0.9875, which was
ca
. 155% higher than that of the stoichiometric
BST
.</description><issn>0002-7820</issn><issn>1551-2916</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><recordid>eNotkMlOwzAQhi0EEqFw4Ql8ZFHS8ZblCFVZpEo9kHvkOGPhqm0iO4C48Qg8I0-CU5jLr9HMNxp9hFwyyFis-UYbzJgsAI5IwpRiKa9YfkwSAOBpUXI4JWchbGLLqlImxC6tRTPS3tLxFenVvaa39MVfz2tHvR5dT_v9YbJzxvcf-h1_vr7Ht71ut0gH3w_oR4dh4iMKWR7hGJLWbk0FNeh1JMM5ObF6G_DiP2ekfljWi6d0tX58XtytUlPkkBYctDUMWNlKg5U1ldZa2La1WPKiQ6EEdJK3OZNSKiG4kryqEFRnurjfihm5-Tsbfw3Bo20G73bafzYMmklQMwlqDoLEL-YiV3M</recordid><startdate>201703</startdate><enddate>201703</enddate><creator>Teranishi, Takashi</creator><creator>Kanemoto, Riku</creator><creator>Hayashi, Hidetaka</creator><creator>Kishimoto, Akira</creator><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>201703</creationdate><title>Effect of the (Ba + Sr)/Ti ratio on the microwave‐tunable properties of Ba 0.6 Sr 0.4 TiO 3 ceramics</title><author>Teranishi, Takashi ; Kanemoto, Riku ; Hayashi, Hidetaka ; Kishimoto, Akira</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c760-720afc1018b4ce9fc9aaa3fbbfe827de3530d42b61444533254299e05dcdce9b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Teranishi, Takashi</creatorcontrib><creatorcontrib>Kanemoto, Riku</creatorcontrib><creatorcontrib>Hayashi, Hidetaka</creatorcontrib><creatorcontrib>Kishimoto, Akira</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of the American Ceramic Society</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Teranishi, Takashi</au><au>Kanemoto, Riku</au><au>Hayashi, Hidetaka</au><au>Kishimoto, Akira</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Effect of the (Ba + Sr)/Ti ratio on the microwave‐tunable properties of Ba 0.6 Sr 0.4 TiO 3 ceramics</atitle><jtitle>Journal of the American Ceramic Society</jtitle><date>2017-03</date><risdate>2017</risdate><volume>100</volume><issue>3</issue><spage>1037</spage><epage>1043</epage><pages>1037-1043</pages><issn>0002-7820</issn><eissn>1551-2916</eissn><abstract>The impact of the (Ba + Sr)/Ti (A/B) ratio on the microwave‐tunable characteristics of diffuse phase transition (
DPT
) ferroelectric Ba
0.6
Sr
0.4
TiO
3
(0.6‐
BST
) ceramics was investigated. The reduction in the lattice constant with increasing nonstoichiometry was attributed to introduced partial Schottky defects, i.e.,
and
. The magnitude of the dielectric constant, ε′, at room temperature in the absence of an applied electric field was governed by the shift in the dielectric maximum temperature,
T
m
, because
T
m
was close to room temperature for the 0.6‐
BST
. The dielectric loss, tanδ, diminished as the ε′ decreased for 0.98≤A/B≤1.05, while the tanδ was much higher for A/B=0.95 having the greatest A‐site vacancy loading. The negatively charged
and
were mainly compensated by oxygen vacancies and likely partly compensated by holes, h
•
, which contributed to the electrical conduction. The tunability,
T
, at 100 MHz was almost constant at 20%–25% for A/B≥1.00 despite the reduction of the ε′, whereas
T
decreased for A/B<1.00 to
ca
. 10% for A/B=0.95 having the greatest A‐site vacancy loading. The results implied that the
for larger A/B values was more efficient in generating nucleation sites in the polar nanoregions (
PNR
s) than the
for smaller A/B values, thereby providing greater dipole polarization. Consequently, the figure of merit,
FOM
, reached its maximum of 250 at A/B=0.9875, which was
ca
. 155% higher than that of the stoichiometric
BST
.</abstract><doi>10.1111/jace.14700</doi><tpages>7</tpages></addata></record> |
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issn | 0002-7820 1551-2916 |
language | eng |
recordid | cdi_crossref_primary_10_1111_jace_14700 |
source | Wiley Online Library Journals Frontfile Complete |
title | Effect of the (Ba + Sr)/Ti ratio on the microwave‐tunable properties of Ba 0.6 Sr 0.4 TiO 3 ceramics |
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