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Proton conducting alkaline earth zirconates and titanates for high drain electrochemical applications
The mobility and stability of protonic defects in acceptor-doped perovskite-type oxides (ABO 3) in the system SrTiO 3–SrZrO 3–BaZrO 3–BaTiO 3 have been examined experimentally and by computational simulations. These materials have the potential to combine high proton conductivity and thermodynamic s...
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Published in: | Solid state ionics 2001-12, Vol.145 (1), p.295-306 |
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creator | Kreuer, K.D. Adams, St Münch, W. Fuchs, A. Klock, U. Maier, J. |
description | The mobility and stability of protonic defects in acceptor-doped perovskite-type oxides (ABO
3) in the system SrTiO
3–SrZrO
3–BaZrO
3–BaTiO
3 have been examined experimentally and by computational simulations. These materials have the potential to combine high proton conductivity and thermodynamic stability. While any structural and chemical perturbation originating from the B-site occupation (poor chemical matching of the acceptor-dopant or Zr/Ti-mixing) leads to a significant reduction of the mobility of protonic defects, Sr/Ba-mixing on the A-site appears to be less critical. The stability of protonic defects is found to essentially scale with the basicity of the lattice oxygen, which is influenced by both A- and B-site occupations. The highest proton conductivities are observed for acceptor-doped BaZrO
3. Despite its significantly higher ionic radius compared to Zr
4+, Y
3+ is found to be optimal as an acceptor dopant for BaZrO
3. Mulliken population analysis shows that Y does not change the oxide's basicity (i.e. it chemically matches on the Zr-site of BaZrO
3). The highest proton conductivities have been observed for high Y-dopant concentrations (15–20 mol%). For temperatures below about 700°C, the observed proton conductivities clearly exceed the oxide ion conductivities of the best oxide ion conductors. The high conductivity and thermodynamic stability make these materials interesting alternatives for oxide ion conductors such as Y-stabilized zirconia, which are currently used as separator material for high drain electrochemical applications, such as solid oxide fuel cells. |
doi_str_mv | 10.1016/S0167-2738(01)00953-5 |
format | article |
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3) in the system SrTiO
3–SrZrO
3–BaZrO
3–BaTiO
3 have been examined experimentally and by computational simulations. These materials have the potential to combine high proton conductivity and thermodynamic stability. While any structural and chemical perturbation originating from the B-site occupation (poor chemical matching of the acceptor-dopant or Zr/Ti-mixing) leads to a significant reduction of the mobility of protonic defects, Sr/Ba-mixing on the A-site appears to be less critical. The stability of protonic defects is found to essentially scale with the basicity of the lattice oxygen, which is influenced by both A- and B-site occupations. The highest proton conductivities are observed for acceptor-doped BaZrO
3. Despite its significantly higher ionic radius compared to Zr
4+, Y
3+ is found to be optimal as an acceptor dopant for BaZrO
3. Mulliken population analysis shows that Y does not change the oxide's basicity (i.e. it chemically matches on the Zr-site of BaZrO
3). The highest proton conductivities have been observed for high Y-dopant concentrations (15–20 mol%). For temperatures below about 700°C, the observed proton conductivities clearly exceed the oxide ion conductivities of the best oxide ion conductors. The high conductivity and thermodynamic stability make these materials interesting alternatives for oxide ion conductors such as Y-stabilized zirconia, which are currently used as separator material for high drain electrochemical applications, such as solid oxide fuel cells.</description><identifier>ISSN: 0167-2738</identifier><identifier>EISSN: 1872-7689</identifier><identifier>DOI: 10.1016/S0167-2738(01)00953-5</identifier><identifier>CODEN: SSIOD3</identifier><language>eng</language><publisher>Amsterdam: Elsevier B.V</publisher><subject>(Ba,Sr)(Zr,Ti)O 3 ; Acceptor-dopant ; Acceptor-doped BaZrO 3 ; Compounds ; Condensed matter: structure, mechanical and thermal properties ; Diffusion in solids ; Exact sciences and technology ; Physics ; Proton conductivity ; Protonic defect ; Self-diffusion and ionic conduction in nonmetals ; SOFC ; SrTiO 3 ; Titatanate ; Transport properties of condensed matter (nonelectronic) ; Zirconate</subject><ispartof>Solid state ionics, 2001-12, Vol.145 (1), p.295-306</ispartof><rights>2001 Elsevier Science B.V.</rights><rights>2002 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c434t-99a20ccc039e83432e4c08999aa1c315f36045d3afd448e718f1849b1f0939523</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>309,310,314,780,784,789,790,23930,23931,25140,27924,27925</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=14116799$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Kreuer, K.D.</creatorcontrib><creatorcontrib>Adams, St</creatorcontrib><creatorcontrib>Münch, W.</creatorcontrib><creatorcontrib>Fuchs, A.</creatorcontrib><creatorcontrib>Klock, U.</creatorcontrib><creatorcontrib>Maier, J.</creatorcontrib><title>Proton conducting alkaline earth zirconates and titanates for high drain electrochemical applications</title><title>Solid state ionics</title><description>The mobility and stability of protonic defects in acceptor-doped perovskite-type oxides (ABO
3) in the system SrTiO
3–SrZrO
3–BaZrO
3–BaTiO
3 have been examined experimentally and by computational simulations. These materials have the potential to combine high proton conductivity and thermodynamic stability. While any structural and chemical perturbation originating from the B-site occupation (poor chemical matching of the acceptor-dopant or Zr/Ti-mixing) leads to a significant reduction of the mobility of protonic defects, Sr/Ba-mixing on the A-site appears to be less critical. The stability of protonic defects is found to essentially scale with the basicity of the lattice oxygen, which is influenced by both A- and B-site occupations. The highest proton conductivities are observed for acceptor-doped BaZrO
3. Despite its significantly higher ionic radius compared to Zr
4+, Y
3+ is found to be optimal as an acceptor dopant for BaZrO
3. Mulliken population analysis shows that Y does not change the oxide's basicity (i.e. it chemically matches on the Zr-site of BaZrO
3). The highest proton conductivities have been observed for high Y-dopant concentrations (15–20 mol%). For temperatures below about 700°C, the observed proton conductivities clearly exceed the oxide ion conductivities of the best oxide ion conductors. The high conductivity and thermodynamic stability make these materials interesting alternatives for oxide ion conductors such as Y-stabilized zirconia, which are currently used as separator material for high drain electrochemical applications, such as solid oxide fuel cells.</description><subject>(Ba,Sr)(Zr,Ti)O 3</subject><subject>Acceptor-dopant</subject><subject>Acceptor-doped BaZrO 3</subject><subject>Compounds</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Diffusion in solids</subject><subject>Exact sciences and technology</subject><subject>Physics</subject><subject>Proton conductivity</subject><subject>Protonic defect</subject><subject>Self-diffusion and ionic conduction in nonmetals</subject><subject>SOFC</subject><subject>SrTiO 3</subject><subject>Titatanate</subject><subject>Transport properties of condensed matter (nonelectronic)</subject><subject>Zirconate</subject><issn>0167-2738</issn><issn>1872-7689</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2001</creationdate><recordtype>article</recordtype><recordid>eNqFkMtKBDEQRYMoOD4-QchG0UVr0kl3JysR8QWCgroOZbraifYkY5IR9OuNjujSTZ7nVlGHkB3ODjnj7dFdWbqq7oTaZ_yAMd2IqlkhE666uupapVfJ5BdZJxspPTPGWqHaCcHbGHLw1AbfL2x2_onC-AKj80gRYp7SDxfLJ2RMFHxPs8uwvA0h0ql7mtI-gvMUR7Q5BjvFmbMwUpjPx3LILvi0RdYGGBNu_-yb5OH87P70srq-ubg6PbmurBQyV1pDzay1TGhUQooapWVKl2fgVvBmEC2TTS9g6KVU2HE1cCX1Ix-YFrqpxSbZW9adx_C6wJTNzCWL4wgewyKZutWs63RbwGYJ2hhSijiYeXQziO-GM_Ml1XxLNV_GDOPmW6ppSm73pwGkMuQQwVuX_sKSl5TWhTteclimfXMYTbIOvcXexaLJ9MH90-kTYgSMtA</recordid><startdate>20011201</startdate><enddate>20011201</enddate><creator>Kreuer, K.D.</creator><creator>Adams, St</creator><creator>Münch, W.</creator><creator>Fuchs, A.</creator><creator>Klock, U.</creator><creator>Maier, J.</creator><general>Elsevier B.V</general><general>Elsevier Science</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>20011201</creationdate><title>Proton conducting alkaline earth zirconates and titanates for high drain electrochemical applications</title><author>Kreuer, K.D. ; Adams, St ; Münch, W. ; Fuchs, A. ; Klock, U. ; Maier, J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c434t-99a20ccc039e83432e4c08999aa1c315f36045d3afd448e718f1849b1f0939523</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2001</creationdate><topic>(Ba,Sr)(Zr,Ti)O 3</topic><topic>Acceptor-dopant</topic><topic>Acceptor-doped BaZrO 3</topic><topic>Compounds</topic><topic>Condensed matter: structure, mechanical and thermal properties</topic><topic>Diffusion in solids</topic><topic>Exact sciences and technology</topic><topic>Physics</topic><topic>Proton conductivity</topic><topic>Protonic defect</topic><topic>Self-diffusion and ionic conduction in nonmetals</topic><topic>SOFC</topic><topic>SrTiO 3</topic><topic>Titatanate</topic><topic>Transport properties of condensed matter (nonelectronic)</topic><topic>Zirconate</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Kreuer, K.D.</creatorcontrib><creatorcontrib>Adams, St</creatorcontrib><creatorcontrib>Münch, W.</creatorcontrib><creatorcontrib>Fuchs, A.</creatorcontrib><creatorcontrib>Klock, U.</creatorcontrib><creatorcontrib>Maier, J.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Solid state ionics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kreuer, K.D.</au><au>Adams, St</au><au>Münch, W.</au><au>Fuchs, A.</au><au>Klock, U.</au><au>Maier, J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Proton conducting alkaline earth zirconates and titanates for high drain electrochemical applications</atitle><jtitle>Solid state ionics</jtitle><date>2001-12-01</date><risdate>2001</risdate><volume>145</volume><issue>1</issue><spage>295</spage><epage>306</epage><pages>295-306</pages><issn>0167-2738</issn><eissn>1872-7689</eissn><coden>SSIOD3</coden><abstract>The mobility and stability of protonic defects in acceptor-doped perovskite-type oxides (ABO
3) in the system SrTiO
3–SrZrO
3–BaZrO
3–BaTiO
3 have been examined experimentally and by computational simulations. These materials have the potential to combine high proton conductivity and thermodynamic stability. While any structural and chemical perturbation originating from the B-site occupation (poor chemical matching of the acceptor-dopant or Zr/Ti-mixing) leads to a significant reduction of the mobility of protonic defects, Sr/Ba-mixing on the A-site appears to be less critical. The stability of protonic defects is found to essentially scale with the basicity of the lattice oxygen, which is influenced by both A- and B-site occupations. The highest proton conductivities are observed for acceptor-doped BaZrO
3. Despite its significantly higher ionic radius compared to Zr
4+, Y
3+ is found to be optimal as an acceptor dopant for BaZrO
3. Mulliken population analysis shows that Y does not change the oxide's basicity (i.e. it chemically matches on the Zr-site of BaZrO
3). The highest proton conductivities have been observed for high Y-dopant concentrations (15–20 mol%). For temperatures below about 700°C, the observed proton conductivities clearly exceed the oxide ion conductivities of the best oxide ion conductors. The high conductivity and thermodynamic stability make these materials interesting alternatives for oxide ion conductors such as Y-stabilized zirconia, which are currently used as separator material for high drain electrochemical applications, such as solid oxide fuel cells.</abstract><cop>Amsterdam</cop><pub>Elsevier B.V</pub><doi>10.1016/S0167-2738(01)00953-5</doi><tpages>12</tpages></addata></record> |
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subjects | (Ba,Sr)(Zr,Ti)O 3 Acceptor-dopant Acceptor-doped BaZrO 3 Compounds Condensed matter: structure, mechanical and thermal properties Diffusion in solids Exact sciences and technology Physics Proton conductivity Protonic defect Self-diffusion and ionic conduction in nonmetals SOFC SrTiO 3 Titatanate Transport properties of condensed matter (nonelectronic) Zirconate |
title | Proton conducting alkaline earth zirconates and titanates for high drain electrochemical applications |
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