Redox behavior and transport properties of La0.5- 2xCexSr0.5+xFeO3- δ and La0.5+2yFe1- yNbyO3- δ perovskites
Identifieur interne : 000229 ( Russie/Analysis ); précédent : 000228; suivant : 000230Redox behavior and transport properties of La0.5- 2xCexSr0.5+xFeO3- δ and La0.5+2yFe1- yNbyO3- δ perovskites
Auteurs : RBID : Pascal:07-0297918Descripteurs français
- Pascal (Inist)
- Propriété transport, Phénomène transport, Dopage, Conductivité mixte, Lanthanide alliage, Superréseau, Conductivité électrique, Solution solide, Effet Mössbauer, Délocalisation électronique, Porteur charge, Non stoechiométrie, Thermogravimétrie, Haute température, Perovskites, Cérium, Fer, Lanthane, Strontium, Perméation, Pouvoir thermoélectrique, Pression partielle, Effet pression, Conductivité type p, Conductivité ionique, Pression atmosphérique, Coefficient dilatation thermique, Addition indium, La, Sr, 8233, 7680.
- Wicri :
English descriptors
- KwdEn :
- Atmospheric pressure, Cerium, Charge carriers, Doping, Electrical conductivity, Electron delocalization, High temperature, Indium additions, Ionic conductivity, Iron, Lanthanum, Mixed conductivity, Moessbauer effect, Nonstoichiometry, P type conductivity, Partial pressure, Permeation, Perovskites, Pressure effects, Rare earth alloys, Solid solutions, Strontium, Superlattices, Thermal expansion coefficient, Thermoelectric power, Thermogravimetry, Transport processes, Transport properties.
Abstract
The effects of doping the mixed-conducting (La,Sr)FeO3-δ system with Ce and Nb have been examined for the solid-solution series, La0.5_2xCe.rSr0.5+xFeO3-δ (x = 0-0.20) and La0.5-2ySr0.5+2yFe1-yNbyO3-δ(y = 0.05-0.10). Mossbauer spectroscopy at 4.1 and 297 K showed that Ce4+ and Nb5+ incorporation suppresses delocalization of p-type electronic charge carriers, whilst oxygen nonstoichiometry of the Ce-containing materials increases. Similar behavior was observed for L0.3Sr0.7Fe0.90Nb0.10-δ at 923-1223 K by coulometric titration and thermogravimetry. High-temperature transport properties were studied with Faradaic efficiency (FE), oxygen-permeation, thermopower and total-conductivity measurements in the oxygen partial pressure range 10-5-0.5 atm. The hole conductivity is lower for the Ce- and Nb-containing perovskites, primarily as a result of the lower Fe4+ concentration. Both dopants decrease oxide-ion conductivity but the effect of Nb-doping on ionic transport is moderate and ion-transference numbers are higher with respect to the Nb-free parent phase, 2.2 x 10∼3 for La0.3Sr0.7Fe0.9Nb0.1O3-δcf. 1.3 x 10 for La0.5Sr0.5FeO3-δ at 1223 K and atmospheric oxygen pressure. The average thermal expansion coefficients calculated from dilatometric data decrease on doping, varying in the range (19.0-21.2) x 10-6K-1 at 780-1080 K.
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<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Redox behavior and transport properties of La<sub>0.5-</sub>
<sub>2x</sub>
Ce<sub>x</sub>
Sr<sub>0.5+x</sub>
FeO<sub>3-</sub>
<sub>δ</sub>
and La<sub>0.5+2y</sub>
Fe<sub>1-</sub>
<sub>y</sub>
Nb<sub>y</sub>
O<sub>3-</sub>
<sub>δ</sub>
perovskites</title>
<author><name sortKey="Kharton, V V" uniqKey="Kharton V">V. V. Kharton</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Ceramics and Glass Engineering, CICECO, University of Aveiro</s1>
<s2>3810-193 Aveiro</s2>
<s3>PRT</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
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<wicri:noRegion>3810-193 Aveiro</wicri:noRegion>
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<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Physicochemical Problems, Belarus State University', 14 Leningradskaya Street</s1>
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<author><name sortKey="Waerenborgh, J C" uniqKey="Waerenborgh J">J. C. Waerenborgh</name>
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<author><name sortKey="Kovalevsky, A V" uniqKey="Kovalevsky A">A. V. Kovalevsky</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Ceramics and Glass Engineering, CICECO, University of Aveiro</s1>
<s2>3810-193 Aveiro</s2>
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<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
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<author><name sortKey="Mather, G C" uniqKey="Mather G">G. C. Mather</name>
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<s2>28049 Madrid</s2>
<s3>ESP</s3>
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<country>Espagne</country>
<placeName><region nuts="2" type="communauté">Communauté de Madrid</region>
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<author><name sortKey="Viskup, A P" uniqKey="Viskup A">A. P. Viskup</name>
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<author><name sortKey="Patrakeev, M V" uniqKey="Patrakeev M">M. V. Patrakeev</name>
<affiliation wicri:level="1"><inist:fA14 i1="05"><s1>Institute of Solid State Chemistry, Ural Division of RAS, 91 Pervomaiskaya Street</s1>
<s2>Ekaterinburg 620219</s2>
<s3>RUS</s3>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>Russie</country>
<wicri:noRegion>Ekaterinburg 620219</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Gaczynski, P" uniqKey="Gaczynski P">P. Gaczynski</name>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Chemistry Department, ITNICFMC-UL, Estrada Nacional 10</s1>
<s2>2686-953 Sacavem</s2>
<s3>PRT</s3>
<sZ>2 aut.</sZ>
<sZ>7 aut.</sZ>
</inist:fA14>
<country>Portugal</country>
<wicri:noRegion>2686-953 Sacavem</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Yaremchenko, A A" uniqKey="Yaremchenko A">A. A. Yaremchenko</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Department of Ceramics and Glass Engineering, CICECO, University of Aveiro</s1>
<s2>3810-193 Aveiro</s2>
<s3>PRT</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>8 aut.</sZ>
</inist:fA14>
<country>Portugal</country>
<wicri:noRegion>3810-193 Aveiro</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Samakhval, V V" uniqKey="Samakhval V">V. V. Samakhval</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Institute of Physicochemical Problems, Belarus State University', 14 Leningradskaya Street</s1>
<s2>220050 Minsk</s2>
<s3>BLR</s3>
<sZ>1 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>9 aut.</sZ>
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<country>Biélorussie</country>
<wicri:noRegion>220050 Minsk</wicri:noRegion>
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<publicationStmt><idno type="inist">07-0297918</idno>
<date when="2007">2007</date>
<idno type="stanalyst">PASCAL 07-0297918 INIST</idno>
<idno type="RBID">Pascal:07-0297918</idno>
<idno type="wicri:Area/Main/Corpus">007B28</idno>
<idno type="wicri:Area/Main/Repository">007186</idno>
<idno type="wicri:Area/Russie/Extraction">000229</idno>
</publicationStmt>
<seriesStmt><idno type="ISSN">1293-2558</idno>
<title level="j" type="abbreviated">Solid state sci.</title>
<title level="j" type="main">Solid state sciences</title>
</seriesStmt>
</fileDesc>
<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Atmospheric pressure</term>
<term>Cerium</term>
<term>Charge carriers</term>
<term>Doping</term>
<term>Electrical conductivity</term>
<term>Electron delocalization</term>
<term>High temperature</term>
<term>Indium additions</term>
<term>Ionic conductivity</term>
<term>Iron</term>
<term>Lanthanum</term>
<term>Mixed conductivity</term>
<term>Moessbauer effect</term>
<term>Nonstoichiometry</term>
<term>P type conductivity</term>
<term>Partial pressure</term>
<term>Permeation</term>
<term>Perovskites</term>
<term>Pressure effects</term>
<term>Rare earth alloys</term>
<term>Solid solutions</term>
<term>Strontium</term>
<term>Superlattices</term>
<term>Thermal expansion coefficient</term>
<term>Thermoelectric power</term>
<term>Thermogravimetry</term>
<term>Transport processes</term>
<term>Transport properties</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Propriété transport</term>
<term>Phénomène transport</term>
<term>Dopage</term>
<term>Conductivité mixte</term>
<term>Lanthanide alliage</term>
<term>Superréseau</term>
<term>Conductivité électrique</term>
<term>Solution solide</term>
<term>Effet Mössbauer</term>
<term>Délocalisation électronique</term>
<term>Porteur charge</term>
<term>Non stoechiométrie</term>
<term>Thermogravimétrie</term>
<term>Haute température</term>
<term>Perovskites</term>
<term>Cérium</term>
<term>Fer</term>
<term>Lanthane</term>
<term>Strontium</term>
<term>Perméation</term>
<term>Pouvoir thermoélectrique</term>
<term>Pression partielle</term>
<term>Effet pression</term>
<term>Conductivité type p</term>
<term>Conductivité ionique</term>
<term>Pression atmosphérique</term>
<term>Coefficient dilatation thermique</term>
<term>Addition indium</term>
<term>La</term>
<term>Sr</term>
<term>8233</term>
<term>7680</term>
</keywords>
<keywords scheme="Wicri" type="concept" xml:lang="fr"><term>Dopage</term>
<term>Fer</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">The effects of doping the mixed-conducting (La,Sr)FeO<sub>3-δ</sub>
system with Ce and Nb have been examined for the solid-solution series, La<sub>0.5_2x</sub>
Ce.rSr<sub>0.5+x</sub>
FeO<sub>3-δ</sub>
(x = 0-0.20) and La<sub>0.5-2y</sub>
Sr<sub>0.5+2y</sub>
Fe<sub>1-y</sub>
Nb<sub>y</sub>
O<sub>3-δ</sub>
(y = 0.05-0.10). Mossbauer spectroscopy at 4.1 and 297 K showed that Ce<sup>4+</sup>
and Nb<sup>5+</sup>
incorporation suppresses delocalization of p-type electronic charge carriers, whilst oxygen nonstoichiometry of the Ce-containing materials increases. Similar behavior was observed for L<sub>0.3</sub>
Sr<sub>0.7</sub>
Fe<sub>0.90</sub>
Nb<sub>0.10-δ</sub>
at 923-1223 K by coulometric titration and thermogravimetry. High-temperature transport properties were studied with Faradaic efficiency (FE), oxygen-permeation, thermopower and total-conductivity measurements in the oxygen partial pressure range 10<sup>-5</sup>
-<sup>0.5</sup>
atm. The hole conductivity is lower for the Ce- and Nb-containing perovskites, primarily as a result of the lower Fe<sup>4+</sup>
concentration. Both dopants decrease oxide-ion conductivity but the effect of Nb-doping on ionic transport is moderate and ion-transference numbers are higher with respect to the Nb-free parent phase, 2.2 x 10<sup>∼3</sup>
for La<sub>0.3</sub>
Sr<sub>0.7</sub>
Fe<sub>0.9</sub>
Nb<sub>0.1</sub>
O<sub>3-δ</sub>
cf. 1.3 x 10 for La<sub>0.5</sub>
Sr<sub>0.5</sub>
FeO<sub>3-δ</sub>
at 1223 K and atmospheric oxygen pressure. The average thermal expansion coefficients calculated from dilatometric data decrease on doping, varying in the range (19.0-21.2) x 10<sup>-6</sup>
K<sup>-1</sup>
at 780-1080 K.</div>
</front>
</TEI>
<inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>1293-2558</s0>
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<fA03 i2="1"><s0>Solid state sci.</s0>
</fA03>
<fA05><s2>9</s2>
</fA05>
<fA06><s2>1</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>Redox behavior and transport properties of La<sub>0.5-</sub>
<sub>2x</sub>
Ce<sub>x</sub>
Sr<sub>0.5+x</sub>
FeO<sub>3-</sub>
<sub>δ</sub>
and La<sub>0.5+2y</sub>
Fe<sub>1-</sub>
<sub>y</sub>
Nb<sub>y</sub>
O<sub>3-</sub>
<sub>δ</sub>
perovskites</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>KHARTON (V. V.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>WAERENBORGH (J. C.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>KOVALEVSKY (A. V.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>MATHER (G. C.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>VISKUP (A. P.)</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>PATRAKEEV (M. V.)</s1>
</fA11>
<fA11 i1="07" i2="1"><s1>GACZYNSKI (P.)</s1>
</fA11>
<fA11 i1="08" i2="1"><s1>YAREMCHENKO (A. A.)</s1>
</fA11>
<fA11 i1="09" i2="1"><s1>SAMAKHVAL (V. V.)</s1>
</fA11>
<fA14 i1="01"><s1>Department of Ceramics and Glass Engineering, CICECO, University of Aveiro</s1>
<s2>3810-193 Aveiro</s2>
<s3>PRT</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>8 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Institute of Physicochemical Problems, Belarus State University', 14 Leningradskaya Street</s1>
<s2>220050 Minsk</s2>
<s3>BLR</s3>
<sZ>1 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>9 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>Chemistry Department, ITNICFMC-UL, Estrada Nacional 10</s1>
<s2>2686-953 Sacavem</s2>
<s3>PRT</s3>
<sZ>2 aut.</sZ>
<sZ>7 aut.</sZ>
</fA14>
<fA14 i1="04"><s1>institute of Ceramics and Glass, CSIC, Cantoblanco</s1>
<s2>28049 Madrid</s2>
<s3>ESP</s3>
<sZ>4 aut.</sZ>
</fA14>
<fA14 i1="05"><s1>Institute of Solid State Chemistry, Ural Division of RAS, 91 Pervomaiskaya Street</s1>
<s2>Ekaterinburg 620219</s2>
<s3>RUS</s3>
<sZ>6 aut.</sZ>
</fA14>
<fA20><s1>32-42</s1>
</fA20>
<fA21><s1>2007</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>11118</s2>
<s5>354000146900780050</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2007 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>35 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>07-0297918</s0>
</fA47>
<fA60><s1>P</s1>
</fA60>
<fA61><s0>A</s0>
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</fA64>
<fA66 i1="01"><s0>FRA</s0>
</fA66>
<fC01 i1="01" l="ENG"><s0>The effects of doping the mixed-conducting (La,Sr)FeO<sub>3-δ</sub>
system with Ce and Nb have been examined for the solid-solution series, La<sub>0.5_2x</sub>
Ce.rSr<sub>0.5+x</sub>
FeO<sub>3-δ</sub>
(x = 0-0.20) and La<sub>0.5-2y</sub>
Sr<sub>0.5+2y</sub>
Fe<sub>1-y</sub>
Nb<sub>y</sub>
O<sub>3-δ</sub>
(y = 0.05-0.10). Mossbauer spectroscopy at 4.1 and 297 K showed that Ce<sup>4+</sup>
and Nb<sup>5+</sup>
incorporation suppresses delocalization of p-type electronic charge carriers, whilst oxygen nonstoichiometry of the Ce-containing materials increases. Similar behavior was observed for L<sub>0.3</sub>
Sr<sub>0.7</sub>
Fe<sub>0.90</sub>
Nb<sub>0.10-δ</sub>
at 923-1223 K by coulometric titration and thermogravimetry. High-temperature transport properties were studied with Faradaic efficiency (FE), oxygen-permeation, thermopower and total-conductivity measurements in the oxygen partial pressure range 10<sup>-5</sup>
-<sup>0.5</sup>
atm. The hole conductivity is lower for the Ce- and Nb-containing perovskites, primarily as a result of the lower Fe<sup>4+</sup>
concentration. Both dopants decrease oxide-ion conductivity but the effect of Nb-doping on ionic transport is moderate and ion-transference numbers are higher with respect to the Nb-free parent phase, 2.2 x 10<sup>∼3</sup>
for La<sub>0.3</sub>
Sr<sub>0.7</sub>
Fe<sub>0.9</sub>
Nb<sub>0.1</sub>
O<sub>3-δ</sub>
cf. 1.3 x 10 for La<sub>0.5</sub>
Sr<sub>0.5</sub>
FeO<sub>3-δ</sub>
at 1223 K and atmospheric oxygen pressure. The average thermal expansion coefficients calculated from dilatometric data decrease on doping, varying in the range (19.0-21.2) x 10<sup>-6</sup>
K<sup>-1</sup>
at 780-1080 K.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70F80</s0>
</fC02>
<fC02 i1="02" i2="X"><s0>001C01A02</s0>
</fC02>
<fC03 i1="01" i2="X" l="FRE"><s0>Propriété transport</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="X" l="ENG"><s0>Transport properties</s0>
<s5>01</s5>
</fC03>
<fC03 i1="01" i2="X" l="SPA"><s0>Propiedad transporte</s0>
<s5>01</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Phénomène transport</s0>
<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Transport processes</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="X" l="FRE"><s0>Dopage</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="X" l="ENG"><s0>Doping</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="X" l="SPA"><s0>Doping</s0>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Conductivité mixte</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Mixed conductivity</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Lanthanide alliage</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Rare earth alloys</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Superréseau</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>Superlattices</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Conductivité électrique</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Electrical conductivity</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Solution solide</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Solid solutions</s0>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Effet Mössbauer</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Moessbauer effect</s0>
<s5>09</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Délocalisation électronique</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Electron delocalization</s0>
<s5>10</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Deslocalización electrónica</s0>
<s5>10</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Porteur charge</s0>
<s5>11</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Charge carriers</s0>
<s5>11</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Non stoechiométrie</s0>
<s5>12</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Nonstoichiometry</s0>
<s5>12</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Thermogravimétrie</s0>
<s5>13</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Thermogravimetry</s0>
<s5>13</s5>
</fC03>
<fC03 i1="14" i2="X" l="FRE"><s0>Haute température</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="X" l="ENG"><s0>High temperature</s0>
<s5>14</s5>
</fC03>
<fC03 i1="14" i2="X" l="SPA"><s0>Alta temperatura</s0>
<s5>14</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Perovskites</s0>
<s5>15</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Perovskites</s0>
<s5>15</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>Cérium</s0>
<s2>NC</s2>
<s5>16</s5>
</fC03>
<fC03 i1="16" i2="3" l="ENG"><s0>Cerium</s0>
<s2>NC</s2>
<s5>16</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Fer</s0>
<s2>NC</s2>
<s5>17</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG"><s0>Iron</s0>
<s2>NC</s2>
<s5>17</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Lanthane</s0>
<s2>NC</s2>
<s5>18</s5>
</fC03>
<fC03 i1="18" i2="3" l="ENG"><s0>Lanthanum</s0>
<s2>NC</s2>
<s5>18</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>Strontium</s0>
<s2>NC</s2>
<s5>19</s5>
</fC03>
<fC03 i1="19" i2="3" l="ENG"><s0>Strontium</s0>
<s2>NC</s2>
<s5>19</s5>
</fC03>
<fC03 i1="20" i2="X" l="FRE"><s0>Perméation</s0>
<s5>29</s5>
</fC03>
<fC03 i1="20" i2="X" l="ENG"><s0>Permeation</s0>
<s5>29</s5>
</fC03>
<fC03 i1="20" i2="X" l="SPA"><s0>Permeación</s0>
<s5>29</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>Pouvoir thermoélectrique</s0>
<s5>30</s5>
</fC03>
<fC03 i1="21" i2="3" l="ENG"><s0>Thermoelectric power</s0>
<s5>30</s5>
</fC03>
<fC03 i1="22" i2="3" l="FRE"><s0>Pression partielle</s0>
<s5>31</s5>
</fC03>
<fC03 i1="22" i2="3" l="ENG"><s0>Partial pressure</s0>
<s5>31</s5>
</fC03>
<fC03 i1="23" i2="3" l="FRE"><s0>Effet pression</s0>
<s5>32</s5>
</fC03>
<fC03 i1="23" i2="3" l="ENG"><s0>Pressure effects</s0>
<s5>32</s5>
</fC03>
<fC03 i1="24" i2="X" l="FRE"><s0>Conductivité type p</s0>
<s5>33</s5>
</fC03>
<fC03 i1="24" i2="X" l="ENG"><s0>P type conductivity</s0>
<s5>33</s5>
</fC03>
<fC03 i1="24" i2="X" l="SPA"><s0>Conductividad tipo p</s0>
<s5>33</s5>
</fC03>
<fC03 i1="25" i2="3" l="FRE"><s0>Conductivité ionique</s0>
<s5>35</s5>
</fC03>
<fC03 i1="25" i2="3" l="ENG"><s0>Ionic conductivity</s0>
<s5>35</s5>
</fC03>
<fC03 i1="26" i2="3" l="FRE"><s0>Pression atmosphérique</s0>
<s5>36</s5>
</fC03>
<fC03 i1="26" i2="3" l="ENG"><s0>Atmospheric pressure</s0>
<s5>36</s5>
</fC03>
<fC03 i1="27" i2="X" l="FRE"><s0>Coefficient dilatation thermique</s0>
<s5>37</s5>
</fC03>
<fC03 i1="27" i2="X" l="ENG"><s0>Thermal expansion coefficient</s0>
<s5>37</s5>
</fC03>
<fC03 i1="27" i2="X" l="SPA"><s0>Coeficiente dilatación térmica</s0>
<s5>37</s5>
</fC03>
<fC03 i1="28" i2="3" l="FRE"><s0>Addition indium</s0>
<s5>38</s5>
</fC03>
<fC03 i1="28" i2="3" l="ENG"><s0>Indium additions</s0>
<s5>38</s5>
</fC03>
<fC03 i1="29" i2="3" l="FRE"><s0>La</s0>
<s4>INC</s4>
<s5>46</s5>
</fC03>
<fC03 i1="30" i2="3" l="FRE"><s0>Sr</s0>
<s4>INC</s4>
<s5>47</s5>
</fC03>
<fC03 i1="31" i2="3" l="FRE"><s0>8233</s0>
<s4>INC</s4>
<s5>65</s5>
</fC03>
<fC03 i1="32" i2="3" l="FRE"><s0>7680</s0>
<s4>INC</s4>
<s5>71</s5>
</fC03>
<fN21><s1>197</s1>
</fN21>
</pA>
</standard>
</inist>
</record>
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