The key role of the composition and structural features in fluoride ion conductivity in tysonite Ce1−xSrxF3−x solid solutionsElectronic supplementary information (ESI) available: Cell parameters, F-(Ce,Sr) distances and additional 19F MAS NMR spectra of Ce1−xSrxF3−x solid solutions. See DOI: 10.1039/c6dt04714a
Pure tysonite-type Ce 1− x Sr x F 3− x solid solutions for 0 ≤ x < 0.15 were prepared by a solid-state route at 900 °C. The cell parameters follow Vegard's laws for 0 ≤ x ≤ 0.10 and the solubility limit is identified (0.10 < x limit < 0.15). For 0 ≤ x ≤ 0.05, the F2-(Ce,Sr) and F3-(Ce,...
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creator | Dieudonné, Belto Chable, Johann Body, Monique Legein, Christophe Durand, Etienne Mauvy, Fabrice Fourcade, Sébastien Leblanc, Marc Maisonneuve, Vincent Demourgues, Alain |
description | Pure tysonite-type Ce
1−
x
Sr
x
F
3−
x
solid solutions for 0 ≤
x
< 0.15 were prepared by a solid-state route at 900 °C. The cell parameters follow Vegard's laws for 0 ≤
x
≤ 0.10 and the solubility limit is identified (0.10 <
x
limit
< 0.15). For 0 ≤
x
≤ 0.05, the F2-(Ce,Sr) and F3-(Ce,Sr) bond distances into [Ce
1−
x
Sr
x
F]
(2−
x
)+
slabs strongly vary with
x
. This slab buckling is maximum around
x
= 0.025 and strongly affects the more mobile F1 fluoride ions located between the slabs. The
19
F MAS NMR spectra show the occurrence of F1-F2,3 exchange at 64 °C. The fraction of mobile F2,3 atoms deduced from the relative intensity of the NMR resonance is maximum for Ce
0.99
Sr
0.01
F
2.99
(22% at 64 °C) while this fraction linearly increases with
x
for La
1−
x
AE
x
F
3−
x
(AE = Ba, Sr). The highest conductivity found for Ce
0.975
Sr
0.025
F
2.975
(3 × 10
−4
S cm
−1
at RT,
E
a
= 0.31 eV) is correlated to the largest dispersion of F2-(Ce,Sr) and F3-(Ce,Sr) distances which induces the maximum sheet buckling. Such a relationship between composition, structural features and fluoride ion conductivity is extended to other tysonite-type fluorides. The key role of the difference between AE
2+
and RE
3+
ionic radii and of the thickness of the slab buckling is established and could allow designing new ionic conductors.
Evolution with
x
of RT ionic conductivity of RE
1−
x
AE
x
F
3−
x
showing that Ce
1−
x
Sr
x
F
3−
x
is the best F
−
tysonite conductor is discussed. |
doi_str_mv | 10.1039/c6dt04714a |
format | Article |
fullrecord | <record><control><sourceid>rsc</sourceid><recordid>TN_cdi_rsc_primary_c6dt04714a</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>c6dt04714a</sourcerecordid><originalsourceid>FETCH-rsc_primary_c6dt04714a3</originalsourceid><addsrcrecordid>eNqFkM1KAzEUhUdRsFY37oXrroW2zp8t7UakdrCLKjjdl2tyB6OZyZBkSvsGrn1En8SkiC4E3SQn3MO530kQnEXhIAqT8SUbchumoyjF_aAVpaNRfxwn6cG3jodHwbExL2EYx-FV3Nq7Xj4TvNIWtJIEqgDr3kyVtTLCClUBVhyM1Q2zjUYJBaETZEBUUMhGacEJvI-pijuTWAu79UO7NaoSlmBK0cfb-ybXmyzxAoySgvuz8QvMTBKz2nkZmKauJZVUWdQ-pFC6xB1FZ5bPu4BrFBKfJE1cqpRQo8aSLGnTg6zfmVIv113gwlismGP07Mj5rohjj8YZLG5yuF88gqn9VvSN_wMcQE4Etw_zCfz-5pPgsEBp6PTrbgfn2Ww5vetrw1a1FqVrsvqxJ-3g4q_5quZF8l_GJw2Gopg</addsrcrecordid><sourcetype>Enrichment Source</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>The key role of the composition and structural features in fluoride ion conductivity in tysonite Ce1−xSrxF3−x solid solutionsElectronic supplementary information (ESI) available: Cell parameters, F-(Ce,Sr) distances and additional 19F MAS NMR spectra of Ce1−xSrxF3−x solid solutions. See DOI: 10.1039/c6dt04714a</title><source>Royal Society Of Chemistry Journals 2008-</source><source>Alma/SFX Local Collection</source><creator>Dieudonné, Belto ; Chable, Johann ; Body, Monique ; Legein, Christophe ; Durand, Etienne ; Mauvy, Fabrice ; Fourcade, Sébastien ; Leblanc, Marc ; Maisonneuve, Vincent ; Demourgues, Alain</creator><creatorcontrib>Dieudonné, Belto ; Chable, Johann ; Body, Monique ; Legein, Christophe ; Durand, Etienne ; Mauvy, Fabrice ; Fourcade, Sébastien ; Leblanc, Marc ; Maisonneuve, Vincent ; Demourgues, Alain</creatorcontrib><description>Pure tysonite-type Ce
1−
x
Sr
x
F
3−
x
solid solutions for 0 ≤
x
< 0.15 were prepared by a solid-state route at 900 °C. The cell parameters follow Vegard's laws for 0 ≤
x
≤ 0.10 and the solubility limit is identified (0.10 <
x
limit
< 0.15). For 0 ≤
x
≤ 0.05, the F2-(Ce,Sr) and F3-(Ce,Sr) bond distances into [Ce
1−
x
Sr
x
F]
(2−
x
)+
slabs strongly vary with
x
. This slab buckling is maximum around
x
= 0.025 and strongly affects the more mobile F1 fluoride ions located between the slabs. The
19
F MAS NMR spectra show the occurrence of F1-F2,3 exchange at 64 °C. The fraction of mobile F2,3 atoms deduced from the relative intensity of the NMR resonance is maximum for Ce
0.99
Sr
0.01
F
2.99
(22% at 64 °C) while this fraction linearly increases with
x
for La
1−
x
AE
x
F
3−
x
(AE = Ba, Sr). The highest conductivity found for Ce
0.975
Sr
0.025
F
2.975
(3 × 10
−4
S cm
−1
at RT,
E
a
= 0.31 eV) is correlated to the largest dispersion of F2-(Ce,Sr) and F3-(Ce,Sr) distances which induces the maximum sheet buckling. Such a relationship between composition, structural features and fluoride ion conductivity is extended to other tysonite-type fluorides. The key role of the difference between AE
2+
and RE
3+
ionic radii and of the thickness of the slab buckling is established and could allow designing new ionic conductors.
Evolution with
x
of RT ionic conductivity of RE
1−
x
AE
x
F
3−
x
showing that Ce
1−
x
Sr
x
F
3−
x
is the best F
−
tysonite conductor is discussed.</description><identifier>ISSN: 1477-9226</identifier><identifier>EISSN: 1477-9234</identifier><identifier>DOI: 10.1039/c6dt04714a</identifier><language>eng</language><creationdate>2017-03</creationdate><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></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>Dieudonné, Belto</creatorcontrib><creatorcontrib>Chable, Johann</creatorcontrib><creatorcontrib>Body, Monique</creatorcontrib><creatorcontrib>Legein, Christophe</creatorcontrib><creatorcontrib>Durand, Etienne</creatorcontrib><creatorcontrib>Mauvy, Fabrice</creatorcontrib><creatorcontrib>Fourcade, Sébastien</creatorcontrib><creatorcontrib>Leblanc, Marc</creatorcontrib><creatorcontrib>Maisonneuve, Vincent</creatorcontrib><creatorcontrib>Demourgues, Alain</creatorcontrib><title>The key role of the composition and structural features in fluoride ion conductivity in tysonite Ce1−xSrxF3−x solid solutionsElectronic supplementary information (ESI) available: Cell parameters, F-(Ce,Sr) distances and additional 19F MAS NMR spectra of Ce1−xSrxF3−x solid solutions. See DOI: 10.1039/c6dt04714a</title><description>Pure tysonite-type Ce
1−
x
Sr
x
F
3−
x
solid solutions for 0 ≤
x
< 0.15 were prepared by a solid-state route at 900 °C. The cell parameters follow Vegard's laws for 0 ≤
x
≤ 0.10 and the solubility limit is identified (0.10 <
x
limit
< 0.15). For 0 ≤
x
≤ 0.05, the F2-(Ce,Sr) and F3-(Ce,Sr) bond distances into [Ce
1−
x
Sr
x
F]
(2−
x
)+
slabs strongly vary with
x
. This slab buckling is maximum around
x
= 0.025 and strongly affects the more mobile F1 fluoride ions located between the slabs. The
19
F MAS NMR spectra show the occurrence of F1-F2,3 exchange at 64 °C. The fraction of mobile F2,3 atoms deduced from the relative intensity of the NMR resonance is maximum for Ce
0.99
Sr
0.01
F
2.99
(22% at 64 °C) while this fraction linearly increases with
x
for La
1−
x
AE
x
F
3−
x
(AE = Ba, Sr). The highest conductivity found for Ce
0.975
Sr
0.025
F
2.975
(3 × 10
−4
S cm
−1
at RT,
E
a
= 0.31 eV) is correlated to the largest dispersion of F2-(Ce,Sr) and F3-(Ce,Sr) distances which induces the maximum sheet buckling. Such a relationship between composition, structural features and fluoride ion conductivity is extended to other tysonite-type fluorides. The key role of the difference between AE
2+
and RE
3+
ionic radii and of the thickness of the slab buckling is established and could allow designing new ionic conductors.
Evolution with
x
of RT ionic conductivity of RE
1−
x
AE
x
F
3−
x
showing that Ce
1−
x
Sr
x
F
3−
x
is the best F
−
tysonite conductor is discussed.</description><issn>1477-9226</issn><issn>1477-9234</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNqFkM1KAzEUhUdRsFY37oXrroW2zp8t7UakdrCLKjjdl2tyB6OZyZBkSvsGrn1En8SkiC4E3SQn3MO530kQnEXhIAqT8SUbchumoyjF_aAVpaNRfxwn6cG3jodHwbExL2EYx-FV3Nq7Xj4TvNIWtJIEqgDr3kyVtTLCClUBVhyM1Q2zjUYJBaETZEBUUMhGacEJvI-pijuTWAu79UO7NaoSlmBK0cfb-ybXmyzxAoySgvuz8QvMTBKz2nkZmKauJZVUWdQ-pFC6xB1FZ5bPu4BrFBKfJE1cqpRQo8aSLGnTg6zfmVIv113gwlismGP07Mj5rohjj8YZLG5yuF88gqn9VvSN_wMcQE4Etw_zCfz-5pPgsEBp6PTrbgfn2Ww5vetrw1a1FqVrsvqxJ-3g4q_5quZF8l_GJw2Gopg</recordid><startdate>20170314</startdate><enddate>20170314</enddate><creator>Dieudonné, Belto</creator><creator>Chable, Johann</creator><creator>Body, Monique</creator><creator>Legein, Christophe</creator><creator>Durand, Etienne</creator><creator>Mauvy, Fabrice</creator><creator>Fourcade, Sébastien</creator><creator>Leblanc, Marc</creator><creator>Maisonneuve, Vincent</creator><creator>Demourgues, Alain</creator><scope/></search><sort><creationdate>20170314</creationdate><title>The key role of the composition and structural features in fluoride ion conductivity in tysonite Ce1−xSrxF3−x solid solutionsElectronic supplementary information (ESI) available: Cell parameters, F-(Ce,Sr) distances and additional 19F MAS NMR spectra of Ce1−xSrxF3−x solid solutions. See DOI: 10.1039/c6dt04714a</title><author>Dieudonné, Belto ; Chable, Johann ; Body, Monique ; Legein, Christophe ; Durand, Etienne ; Mauvy, Fabrice ; Fourcade, Sébastien ; Leblanc, Marc ; Maisonneuve, Vincent ; Demourgues, Alain</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-rsc_primary_c6dt04714a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Dieudonné, Belto</creatorcontrib><creatorcontrib>Chable, Johann</creatorcontrib><creatorcontrib>Body, Monique</creatorcontrib><creatorcontrib>Legein, Christophe</creatorcontrib><creatorcontrib>Durand, Etienne</creatorcontrib><creatorcontrib>Mauvy, Fabrice</creatorcontrib><creatorcontrib>Fourcade, Sébastien</creatorcontrib><creatorcontrib>Leblanc, Marc</creatorcontrib><creatorcontrib>Maisonneuve, Vincent</creatorcontrib><creatorcontrib>Demourgues, Alain</creatorcontrib></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Dieudonné, Belto</au><au>Chable, Johann</au><au>Body, Monique</au><au>Legein, Christophe</au><au>Durand, Etienne</au><au>Mauvy, Fabrice</au><au>Fourcade, Sébastien</au><au>Leblanc, Marc</au><au>Maisonneuve, Vincent</au><au>Demourgues, Alain</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The key role of the composition and structural features in fluoride ion conductivity in tysonite Ce1−xSrxF3−x solid solutionsElectronic supplementary information (ESI) available: Cell parameters, F-(Ce,Sr) distances and additional 19F MAS NMR spectra of Ce1−xSrxF3−x solid solutions. See DOI: 10.1039/c6dt04714a</atitle><date>2017-03-14</date><risdate>2017</risdate><volume>46</volume><issue>11</issue><spage>3761</spage><epage>3769</epage><pages>3761-3769</pages><issn>1477-9226</issn><eissn>1477-9234</eissn><abstract>Pure tysonite-type Ce
1−
x
Sr
x
F
3−
x
solid solutions for 0 ≤
x
< 0.15 were prepared by a solid-state route at 900 °C. The cell parameters follow Vegard's laws for 0 ≤
x
≤ 0.10 and the solubility limit is identified (0.10 <
x
limit
< 0.15). For 0 ≤
x
≤ 0.05, the F2-(Ce,Sr) and F3-(Ce,Sr) bond distances into [Ce
1−
x
Sr
x
F]
(2−
x
)+
slabs strongly vary with
x
. This slab buckling is maximum around
x
= 0.025 and strongly affects the more mobile F1 fluoride ions located between the slabs. The
19
F MAS NMR spectra show the occurrence of F1-F2,3 exchange at 64 °C. The fraction of mobile F2,3 atoms deduced from the relative intensity of the NMR resonance is maximum for Ce
0.99
Sr
0.01
F
2.99
(22% at 64 °C) while this fraction linearly increases with
x
for La
1−
x
AE
x
F
3−
x
(AE = Ba, Sr). The highest conductivity found for Ce
0.975
Sr
0.025
F
2.975
(3 × 10
−4
S cm
−1
at RT,
E
a
= 0.31 eV) is correlated to the largest dispersion of F2-(Ce,Sr) and F3-(Ce,Sr) distances which induces the maximum sheet buckling. Such a relationship between composition, structural features and fluoride ion conductivity is extended to other tysonite-type fluorides. The key role of the difference between AE
2+
and RE
3+
ionic radii and of the thickness of the slab buckling is established and could allow designing new ionic conductors.
Evolution with
x
of RT ionic conductivity of RE
1−
x
AE
x
F
3−
x
showing that Ce
1−
x
Sr
x
F
3−
x
is the best F
−
tysonite conductor is discussed.</abstract><doi>10.1039/c6dt04714a</doi><tpages>9</tpages></addata></record> |
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source | Royal Society Of Chemistry Journals 2008-; Alma/SFX Local Collection |
title | The key role of the composition and structural features in fluoride ion conductivity in tysonite Ce1−xSrxF3−x solid solutionsElectronic supplementary information (ESI) available: Cell parameters, F-(Ce,Sr) distances and additional 19F MAS NMR spectra of Ce1−xSrxF3−x solid solutions. See DOI: 10.1039/c6dt04714a |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-20T14%3A34%3A47IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-rsc&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=The%20key%20role%20of%20the%20composition%20and%20structural%20features%20in%20fluoride%20ion%20conductivity%20in%20tysonite%20Ce1%E2%88%92xSrxF3%E2%88%92x%20solid%20solutionsElectronic%20supplementary%20information%20(ESI)%20available:%20Cell%20parameters,%20F-(Ce,Sr)%20distances%20and%20additional%2019F%20MAS%20NMR%20spectra%20of%20Ce1%E2%88%92xSrxF3%E2%88%92x%20solid%20solutions.%20See%20DOI:%2010.1039/c6dt04714a&rft.au=Dieudonn%C3%A9,%20Belto&rft.date=2017-03-14&rft.volume=46&rft.issue=11&rft.spage=3761&rft.epage=3769&rft.pages=3761-3769&rft.issn=1477-9226&rft.eissn=1477-9234&rft_id=info:doi/10.1039/c6dt04714a&rft_dat=%3Crsc%3Ec6dt04714a%3C/rsc%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 |