Development of nanoimprinted InP QDs decorated polyaniline solar cell with conversion efficiency 3%
Identifieur interne : 000F42 ( Main/Repository ); précédent : 000F41; suivant : 000F43Development of nanoimprinted InP QDs decorated polyaniline solar cell with conversion efficiency 3%
Auteurs : RBID : Pascal:13-0345453Descripteurs français
- Pascal (Inist)
- Nanolithographie, Nanoimpression, Cellule solaire, Taux conversion, Application industrielle, Multidisciplinaire, Dispositif optoélectronique, Recombinaison non radiative, Transfert énergie, Transfert charge, Recombinaison porteur charge, Diffusion(transport), Exciton, Microstructure, Morphologie, Nanostructure, Moniteur, Modèle cinétique, Méthode temps vol, Epaisseur, Rayonnement UV extrême, Phosphure d'indium, Composé binaire, Aniline polymère, Matériau hybride organique minéral, Nanoparticule, Nanocomposite, Point quantique semiconducteur, Polymère conjugué, Point quantique, Fabrication microélectronique, 8116N, 8235C, 8460J, 8107B, InP, 6630P, 66, 7135, 6865, 8107T, 8535B, 8540H.
English descriptors
- KwdEn :
- Aniline polymer, Binary compound, Charge carrier recombination, Charge transfer, Conjugated polymer, Conversion rate, Diffusion, Energy transfer, Exciton, Indium phosphide, Industrial application, Kinetic model, Microelectronic fabrication, Microstructure, Monitor, Morphology, Multidisciplinary, Nanocomposite, Nanoimprint, Nanolithography, Nanoparticle, Nanostructure, Non radiative recombination, Optoelectronic device, Organic-inorganic hybrid materials, Quantum dot, Semiconductor quantum dots, Solar cell, Thickness, Time of flight method, Vacuum ultraviolet radiation.
Abstract
Organic-inorganic hybrid materials received considerable attention due to promising industrial applications. The originality of novel chemical recipes, allowing incorporation of well-defined nanoparticle structures into complex hybrid architectures, opens new possibilities for multidisciplinary fields and in particular in optoelectronic devices. The rate of non-radiative recombination and energy transfer through a hybrid inorganic/organic nano-composite is mainly governing the ability of charge transfer from semiconductor quantum dots to conjugated polymers. Herein, we report that the electron-hole non-radiative recombination in polymer can be constricted by funneling the diffusion of exciton by engineering a proper morphology of a hybrid nanostructure. InP quantum dots have been selected due to their efficient exciton generation and polyaniline as a conjugated polymer for its potency to suppress non-radiative recombination by restraining exciton diffusion. The hole transfer was monitored via bi-exponential kinetic model and time of flight method. The conversion efficiency of the prepared films increased from 0.23% to 3.1% when the thickness is increased from 14 nm to 157 nm.
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<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Development of nanoimprinted InP QDs decorated polyaniline solar cell with conversion efficiency 3%</title><author><name sortKey="Mahmoud, Waleed E" uniqKey="Mahmoud W">Waleed E. Mahmoud</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>King Abdulaziz University, Faculty of Science, Physics Department</s1><s2>Jeddah</s2><s3>SAU</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Arabie saoudite</country><wicri:noRegion>Jeddah</wicri:noRegion></affiliation></author><author><name sortKey="Chang, Y C" uniqKey="Chang Y">Y. C. Chang</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>King Abdulaziz University, Faculty of Science, Physics Department</s1><s2>Jeddah</s2><s3>SAU</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Arabie saoudite</country><wicri:noRegion>Jeddah</wicri:noRegion></affiliation><affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Research Center for Applied Sciences, Academia Sinica, Academia Road, Nankang</s1><s2>Taipei 115</s2><s3>TWN</s3><sZ>2 aut.</sZ></inist:fA14><country>Taïwan</country><wicri:noRegion>Taipei 115</wicri:noRegion></affiliation></author><author><name sortKey="Al Ghamdi, A A" uniqKey="Al Ghamdi A">A. A. Al-Ghamdi</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>King Abdulaziz University, Faculty of Science, Physics Department</s1><s2>Jeddah</s2><s3>SAU</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Arabie saoudite</country><wicri:noRegion>Jeddah</wicri:noRegion></affiliation></author><author><name sortKey="Al Marzouki, F" uniqKey="Al Marzouki F">F. Al-Marzouki</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>King Abdulaziz University, Faculty of Science, Physics Department</s1><s2>Jeddah</s2><s3>SAU</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Arabie saoudite</country><wicri:noRegion>Jeddah</wicri:noRegion></affiliation></author><author><name sortKey="Bronstein, Lyudmila M" uniqKey="Bronstein L">Lyudmila M. Bronstein</name><affiliation wicri:level="1"><inist:fA14 i1="01"><s1>King Abdulaziz University, Faculty of Science, Physics Department</s1><s2>Jeddah</s2><s3>SAU</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Arabie saoudite</country><wicri:noRegion>Jeddah</wicri:noRegion></affiliation><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Indiana University, Department of Chemistry</s1><s2>Bloomington, IN 47405</s2><s3>USA</s3><sZ>5 aut.</sZ></inist:fA14><country>États-Unis</country><wicri:noRegion>Bloomington, IN 47405</wicri:noRegion></affiliation></author></titleStmt><publicationStmt><idno type="inist">13-0345453</idno><date when="2013">2013</date><idno type="stanalyst">PASCAL 13-0345453 INIST</idno><idno type="RBID">Pascal:13-0345453</idno><idno type="wicri:Area/Main/Corpus">000564</idno><idno type="wicri:Area/Main/Repository">000F42</idno></publicationStmt><seriesStmt><idno type="ISSN">1566-1199</idno><title level="j" type="abbreviated">Org. electron. : (Print)</title><title level="j" type="main">Organic electronics : (Print)</title></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Aniline polymer</term><term>Binary compound</term><term>Charge carrier recombination</term><term>Charge transfer</term><term>Conjugated polymer</term><term>Conversion rate</term><term>Diffusion</term><term>Energy transfer</term><term>Exciton</term><term>Indium phosphide</term><term>Industrial application</term><term>Kinetic model</term><term>Microelectronic fabrication</term><term>Microstructure</term><term>Monitor</term><term>Morphology</term><term>Multidisciplinary</term><term>Nanocomposite</term><term>Nanoimprint</term><term>Nanolithography</term><term>Nanoparticle</term><term>Nanostructure</term><term>Non radiative recombination</term><term>Optoelectronic device</term><term>Organic-inorganic hybrid materials</term><term>Quantum dot</term><term>Semiconductor quantum dots</term><term>Solar cell</term><term>Thickness</term><term>Time of flight method</term><term>Vacuum ultraviolet radiation</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Nanolithographie</term><term>Nanoimpression</term><term>Cellule solaire</term><term>Taux conversion</term><term>Application industrielle</term><term>Multidisciplinaire</term><term>Dispositif optoélectronique</term><term>Recombinaison non radiative</term><term>Transfert énergie</term><term>Transfert charge</term><term>Recombinaison porteur charge</term><term>Diffusion(transport)</term><term>Exciton</term><term>Microstructure</term><term>Morphologie</term><term>Nanostructure</term><term>Moniteur</term><term>Modèle cinétique</term><term>Méthode temps vol</term><term>Epaisseur</term><term>Rayonnement UV extrême</term><term>Phosphure d'indium</term><term>Composé binaire</term><term>Aniline polymère</term><term>Matériau hybride organique minéral</term><term>Nanoparticule</term><term>Nanocomposite</term><term>Point quantique semiconducteur</term><term>Polymère conjugué</term><term>Point quantique</term><term>Fabrication microélectronique</term><term>8116N</term><term>8235C</term><term>8460J</term><term>8107B</term><term>InP</term><term>6630P</term><term>66</term><term>7135</term><term>6865</term><term>8107T</term><term>8535B</term><term>8540H</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">Organic-inorganic hybrid materials received considerable attention due to promising industrial applications. The originality of novel chemical recipes, allowing incorporation of well-defined nanoparticle structures into complex hybrid architectures, opens new possibilities for multidisciplinary fields and in particular in optoelectronic devices. The rate of non-radiative recombination and energy transfer through a hybrid inorganic/organic nano-composite is mainly governing the ability of charge transfer from semiconductor quantum dots to conjugated polymers. Herein, we report that the electron-hole non-radiative recombination in polymer can be constricted by funneling the diffusion of exciton by engineering a proper morphology of a hybrid nanostructure. InP quantum dots have been selected due to their efficient exciton generation and polyaniline as a conjugated polymer for its potency to suppress non-radiative recombination by restraining exciton diffusion. The hole transfer was monitored via bi-exponential kinetic model and time of flight method. The conversion efficiency of the prepared films increased from 0.23% to 3.1% when the thickness is increased from 14 nm to 157 nm.</div></front></TEI><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>1566-1199</s0></fA01><fA03 i2="1"><s0>Org. electron. : (Print)</s0></fA03><fA05><s2>14</s2></fA05><fA06><s2>11</s2></fA06><fA08 i1="01" i2="1" l="ENG"><s1>Development of nanoimprinted InP QDs decorated polyaniline solar cell with conversion efficiency 3%</s1></fA08><fA11 i1="01" i2="1"><s1>MAHMOUD (Waleed E.)</s1></fA11><fA11 i1="02" i2="1"><s1>CHANG (Y. C.)</s1></fA11><fA11 i1="03" i2="1"><s1>AL-GHAMDI (A. A.)</s1></fA11><fA11 i1="04" i2="1"><s1>AL-MARZOUKI (F.)</s1></fA11><fA11 i1="05" i2="1"><s1>BRONSTEIN (Lyudmila M.)</s1></fA11><fA14 i1="01"><s1>King Abdulaziz University, Faculty of Science, Physics Department</s1><s2>Jeddah</s2><s3>SAU</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></fA14><fA14 i1="02"><s1>Research Center for Applied Sciences, Academia Sinica, Academia Road, Nankang</s1><s2>Taipei 115</s2><s3>TWN</s3><sZ>2 aut.</sZ></fA14><fA14 i1="03"><s1>Indiana University, Department of Chemistry</s1><s2>Bloomington, IN 47405</s2><s3>USA</s3><sZ>5 aut.</sZ></fA14><fA20><s1>2762-2769</s1></fA20><fA21><s1>2013</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>27255</s2><s5>354000501043310080</s5></fA43><fA44><s0>0000</s0><s1>© 2013 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>45 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>13-0345453</s0></fA47><fA60><s1>P</s1></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>Organic electronics : (Print)</s0></fA64><fA66 i1="01"><s0>NLD</s0></fA66><fC01 i1="01" l="ENG"><s0>Organic-inorganic hybrid materials received considerable attention due to promising industrial applications. The originality of novel chemical recipes, allowing incorporation of well-defined nanoparticle structures into complex hybrid architectures, opens new possibilities for multidisciplinary fields and in particular in optoelectronic devices. The rate of non-radiative recombination and energy transfer through a hybrid inorganic/organic nano-composite is mainly governing the ability of charge transfer from semiconductor quantum dots to conjugated polymers. Herein, we report that the electron-hole non-radiative recombination in polymer can be constricted by funneling the diffusion of exciton by engineering a proper morphology of a hybrid nanostructure. InP quantum dots have been selected due to their efficient exciton generation and polyaniline as a conjugated polymer for its potency to suppress non-radiative recombination by restraining exciton diffusion. The hole transfer was monitored via bi-exponential kinetic model and time of flight method. The conversion efficiency of the prepared films increased from 0.23% to 3.1% when the thickness is increased from 14 nm to 157 nm.</s0></fC01><fC02 i1="01" i2="X"><s0>001D03F17</s0></fC02><fC02 i1="02" i2="3"><s0>001B80A16R</s0></fC02><fC02 i1="03" i2="X"><s0>001D03F15</s0></fC02><fC02 i1="04" i2="X"><s0>001D06C02D1</s0></fC02><fC02 i1="05" i2="X"><s0>230</s0></fC02><fC03 i1="01" i2="3" l="FRE"><s0>Nanolithographie</s0><s5>01</s5></fC03><fC03 i1="01" i2="3" l="ENG"><s0>Nanolithography</s0><s5>01</s5></fC03><fC03 i1="02" i2="X" l="FRE"><s0>Nanoimpression</s0><s5>02</s5></fC03><fC03 i1="02" i2="X" l="ENG"><s0>Nanoimprint</s0><s5>02</s5></fC03><fC03 i1="02" i2="X" l="SPA"><s0>Nanoimpresión</s0><s5>02</s5></fC03><fC03 i1="03" i2="X" l="FRE"><s0>Cellule solaire</s0><s5>03</s5></fC03><fC03 i1="03" i2="X" l="ENG"><s0>Solar cell</s0><s5>03</s5></fC03><fC03 i1="03" i2="X" l="SPA"><s0>Célula solar</s0><s5>03</s5></fC03><fC03 i1="04" i2="X" l="FRE"><s0>Taux conversion</s0><s5>04</s5></fC03><fC03 i1="04" i2="X" l="ENG"><s0>Conversion rate</s0><s5>04</s5></fC03><fC03 i1="04" i2="X" l="SPA"><s0>Factor conversión</s0><s5>04</s5></fC03><fC03 i1="05" i2="X" l="FRE"><s0>Application industrielle</s0><s5>05</s5></fC03><fC03 i1="05" i2="X" l="ENG"><s0>Industrial application</s0><s5>05</s5></fC03><fC03 i1="05" i2="X" l="SPA"><s0>Aplicación industrial</s0><s5>05</s5></fC03><fC03 i1="06" i2="X" l="FRE"><s0>Multidisciplinaire</s0><s5>06</s5></fC03><fC03 i1="06" i2="X" l="ENG"><s0>Multidisciplinary</s0><s5>06</s5></fC03><fC03 i1="06" i2="X" l="SPA"><s0>Multidisciplinar</s0><s5>06</s5></fC03><fC03 i1="07" i2="X" l="FRE"><s0>Dispositif optoélectronique</s0><s5>07</s5></fC03><fC03 i1="07" i2="X" l="ENG"><s0>Optoelectronic device</s0><s5>07</s5></fC03><fC03 i1="07" i2="X" l="SPA"><s0>Dispositivo optoelectrónico</s0><s5>07</s5></fC03><fC03 i1="08" i2="X" l="FRE"><s0>Recombinaison non radiative</s0><s5>08</s5></fC03><fC03 i1="08" i2="X" l="ENG"><s0>Non radiative recombination</s0><s5>08</s5></fC03><fC03 i1="08" i2="X" l="SPA"><s0>Recombinación no radiativa</s0><s5>08</s5></fC03><fC03 i1="09" i2="X" l="FRE"><s0>Transfert énergie</s0><s5>09</s5></fC03><fC03 i1="09" i2="X" l="ENG"><s0>Energy transfer</s0><s5>09</s5></fC03><fC03 i1="09" i2="X" l="SPA"><s0>Transferencia energía</s0><s5>09</s5></fC03><fC03 i1="10" i2="X" l="FRE"><s0>Transfert charge</s0><s5>10</s5></fC03><fC03 i1="10" i2="X" l="ENG"><s0>Charge transfer</s0><s5>10</s5></fC03><fC03 i1="10" i2="X" l="SPA"><s0>Transferencia carga</s0><s5>10</s5></fC03><fC03 i1="11" i2="X" l="FRE"><s0>Recombinaison porteur charge</s0><s5>11</s5></fC03><fC03 i1="11" i2="X" l="ENG"><s0>Charge carrier recombination</s0><s5>11</s5></fC03><fC03 i1="11" i2="X" l="SPA"><s0>Recombinación portador carga</s0><s5>11</s5></fC03><fC03 i1="12" i2="3" l="FRE"><s0>Diffusion(transport)</s0><s5>12</s5></fC03><fC03 i1="12" i2="3" l="ENG"><s0>Diffusion</s0><s5>12</s5></fC03><fC03 i1="13" i2="X" l="FRE"><s0>Exciton</s0><s5>13</s5></fC03><fC03 i1="13" i2="X" l="ENG"><s0>Exciton</s0><s5>13</s5></fC03><fC03 i1="13" i2="X" l="SPA"><s0>Excitón</s0><s5>13</s5></fC03><fC03 i1="14" i2="X" l="FRE"><s0>Microstructure</s0><s5>14</s5></fC03><fC03 i1="14" i2="X" l="ENG"><s0>Microstructure</s0><s5>14</s5></fC03><fC03 i1="14" i2="X" l="SPA"><s0>Microestructura</s0><s5>14</s5></fC03><fC03 i1="15" i2="X" l="FRE"><s0>Morphologie</s0><s5>15</s5></fC03><fC03 i1="15" i2="X" l="ENG"><s0>Morphology</s0><s5>15</s5></fC03><fC03 i1="15" i2="X" l="SPA"><s0>Morfología</s0><s5>15</s5></fC03><fC03 i1="16" i2="X" l="FRE"><s0>Nanostructure</s0><s5>16</s5></fC03><fC03 i1="16" i2="X" l="ENG"><s0>Nanostructure</s0><s5>16</s5></fC03><fC03 i1="16" i2="X" l="SPA"><s0>Nanoestructura</s0><s5>16</s5></fC03><fC03 i1="17" i2="X" l="FRE"><s0>Moniteur</s0><s5>17</s5></fC03><fC03 i1="17" i2="X" l="ENG"><s0>Monitor</s0><s5>17</s5></fC03><fC03 i1="17" i2="X" l="SPA"><s0>Monitor</s0><s5>17</s5></fC03><fC03 i1="18" i2="X" l="FRE"><s0>Modèle cinétique</s0><s5>18</s5></fC03><fC03 i1="18" i2="X" l="ENG"><s0>Kinetic model</s0><s5>18</s5></fC03><fC03 i1="18" i2="X" l="SPA"><s0>Modelo cinético</s0><s5>18</s5></fC03><fC03 i1="19" i2="X" l="FRE"><s0>Méthode temps vol</s0><s5>19</s5></fC03><fC03 i1="19" i2="X" l="ENG"><s0>Time of flight method</s0><s5>19</s5></fC03><fC03 i1="19" i2="X" l="SPA"><s0>Método tiempo vuelo</s0><s5>19</s5></fC03><fC03 i1="20" i2="X" l="FRE"><s0>Epaisseur</s0><s5>20</s5></fC03><fC03 i1="20" i2="X" l="ENG"><s0>Thickness</s0><s5>20</s5></fC03><fC03 i1="20" i2="X" l="SPA"><s0>Espesor</s0><s5>20</s5></fC03><fC03 i1="21" i2="X" l="FRE"><s0>Rayonnement UV extrême</s0><s5>21</s5></fC03><fC03 i1="21" i2="X" l="ENG"><s0>Vacuum ultraviolet radiation</s0><s5>21</s5></fC03><fC03 i1="21" i2="X" l="SPA"><s0>Radiación ultravioleta extrema</s0><s5>21</s5></fC03><fC03 i1="22" i2="X" l="FRE"><s0>Phosphure d'indium</s0><s5>22</s5></fC03><fC03 i1="22" i2="X" l="ENG"><s0>Indium phosphide</s0><s5>22</s5></fC03><fC03 i1="22" i2="X" l="SPA"><s0>Indio fosfuro</s0><s5>22</s5></fC03><fC03 i1="23" i2="X" l="FRE"><s0>Composé binaire</s0><s5>23</s5></fC03><fC03 i1="23" i2="X" l="ENG"><s0>Binary compound</s0><s5>23</s5></fC03><fC03 i1="23" i2="X" l="SPA"><s0>Compuesto binario</s0><s5>23</s5></fC03><fC03 i1="24" i2="X" l="FRE"><s0>Aniline polymère</s0><s2>NK</s2><s5>24</s5></fC03><fC03 i1="24" i2="X" l="ENG"><s0>Aniline polymer</s0><s2>NK</s2><s5>24</s5></fC03><fC03 i1="24" i2="X" l="SPA"><s0>Anilina polímero</s0><s2>NK</s2><s5>24</s5></fC03><fC03 i1="25" i2="3" l="FRE"><s0>Matériau hybride organique minéral</s0><s5>25</s5></fC03><fC03 i1="25" i2="3" l="ENG"><s0>Organic-inorganic hybrid materials</s0><s5>25</s5></fC03><fC03 i1="26" i2="X" l="FRE"><s0>Nanoparticule</s0><s5>26</s5></fC03><fC03 i1="26" i2="X" l="ENG"><s0>Nanoparticle</s0><s5>26</s5></fC03><fC03 i1="26" i2="X" l="SPA"><s0>Nanopartícula</s0><s5>26</s5></fC03><fC03 i1="27" i2="X" l="FRE"><s0>Nanocomposite</s0><s5>27</s5></fC03><fC03 i1="27" i2="X" l="ENG"><s0>Nanocomposite</s0><s5>27</s5></fC03><fC03 i1="27" i2="X" l="SPA"><s0>Nanocompuesto</s0><s5>27</s5></fC03><fC03 i1="28" i2="3" l="FRE"><s0>Point quantique semiconducteur</s0><s5>28</s5></fC03><fC03 i1="28" i2="3" l="ENG"><s0>Semiconductor quantum dots</s0><s5>28</s5></fC03><fC03 i1="29" i2="X" l="FRE"><s0>Polymère conjugué</s0><s5>29</s5></fC03><fC03 i1="29" i2="X" l="ENG"><s0>Conjugated polymer</s0><s5>29</s5></fC03><fC03 i1="29" i2="X" l="SPA"><s0>Polímero conjugado</s0><s5>29</s5></fC03><fC03 i1="30" i2="X" l="FRE"><s0>Point quantique</s0><s5>30</s5></fC03><fC03 i1="30" i2="X" l="ENG"><s0>Quantum dot</s0><s5>30</s5></fC03><fC03 i1="30" i2="X" l="SPA"><s0>Punto cuántico</s0><s5>30</s5></fC03><fC03 i1="31" i2="X" l="FRE"><s0>Fabrication microélectronique</s0><s5>46</s5></fC03><fC03 i1="31" i2="X" l="ENG"><s0>Microelectronic fabrication</s0><s5>46</s5></fC03><fC03 i1="31" i2="X" l="SPA"><s0>Fabricación microeléctrica</s0><s5>46</s5></fC03><fC03 i1="32" i2="X" l="FRE"><s0>8116N</s0><s4>INC</s4><s5>56</s5></fC03><fC03 i1="33" i2="X" l="FRE"><s0>8235C</s0><s4>INC</s4><s5>57</s5></fC03><fC03 i1="34" i2="X" l="FRE"><s0>8460J</s0><s4>INC</s4><s5>58</s5></fC03><fC03 i1="35" i2="X" l="FRE"><s0>8107B</s0><s4>INC</s4><s5>59</s5></fC03><fC03 i1="36" i2="X" l="FRE"><s0>InP</s0><s4>INC</s4><s5>82</s5></fC03><fC03 i1="37" i2="X" l="FRE"><s0>6630P</s0><s4>INC</s4><s5>83</s5></fC03><fC03 i1="38" i2="X" l="FRE"><s0>66</s0><s4>INC</s4><s5>84</s5></fC03><fC03 i1="39" i2="X" l="FRE"><s0>7135</s0><s4>INC</s4><s5>85</s5></fC03><fC03 i1="40" i2="X" l="FRE"><s0>6865</s0><s4>INC</s4><s5>86</s5></fC03><fC03 i1="41" i2="X" l="FRE"><s0>8107T</s0><s4>INC</s4><s5>87</s5></fC03><fC03 i1="42" i2="X" l="FRE"><s0>8535B</s0><s4>INC</s4><s5>88</s5></fC03><fC03 i1="43" i2="X" l="FRE"><s0>8540H</s0><s4>INC</s4><s5>89</s5></fC03><fN21><s1>329</s1></fN21><fN44 i1="01"><s1>OTO</s1></fN44><fN82><s1>OTO</s1></fN82></pA></standard></inist></record>Pour manipuler ce document sous Unix (Dilib)
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