A Comparative First-Principles Study of Fe-, Co-and FeCo-Doped ZnO with Wurtzite and Zinc Blende Structures
Identifieur interne : 000057 ( PascalFrancis/Checkpoint ); précédent : 000056; suivant : 000058A Comparative First-Principles Study of Fe-, Co-and FeCo-Doped ZnO with Wurtzite and Zinc Blende Structures
Auteurs : N. Mamouni [Maroc] ; A. Benyoussef [Maroc] ; A. El Kenz [Maroc] ; H. Ez-Zahraouy [Maroc] ; M. Loulidi [Maroc] ; E. H. Saidi [Maroc] ; M. Bououdina [Bahreïn]Source :
- Journal of superconductivity and novel magnetism [ 1557-1939 ] ; 2012.
Descripteurs français
- Pascal (Inist)
- Méthode fonctionnelle densité, Codopage, Structure électronique, Addition fer, Addition cobalt, Semimétal, Densité état électron, Ferromagnétisme, Interaction échange, Calcul ab initio, Bande impureté, Moment magnétique, Semiconducteur semimagnétique, Oxyde de zinc, Structure blende, Structure wurtzite, Matériau diamagnétique, Matériau ferromagnétique, ZnO.
English descriptors
- KwdEn :
- Ab initio calculations, Blende structure, Cobalt additions, Codoping, Density functional method, Diamagnetic materials, Electronic density of states, Electronic structure, Exchange interactions, Ferromagnetic materials, Ferromagnetism, Impurity bands, Iron additions, Magnetic moments, Semimagnetic semiconductors, Semimetals, Wurtzite structure, Zinc oxide.
Abstract
First-principles study of the electronic and magnetic properties of zinc-blende and wurtzite structures of Fe-, Co-, and FeCo-doped ZnO is presented. It is found that after doping, this diamagnetic material becomes ferromagnetic and half-metallic. It is also shown that the half-metallicity may be obtained for ZnFeO, ZnCoO, and ZnFe-CoO. The analysis of the spin density reveals that the ferromagnetic phase is due to the ferromagnetic coupling between the p-d states. The effects of Fe on the magnetic properties of ZB and WZ Fe-doped ZnO compound have been investigated with the GGA calculations. In order to understand the role of Fe atom in the ferromagnetism, the density of states both in the presence and absence of Co doping, were calculated. The obtained results show the presence of coupling between Co and Fe atoms through the spin-split impurity band exchange mechanism. More importantly, the calculations show that the magnetic moment changes sensitively with the type of structure of ZnO, zinc-blende, or wurtzite. A discussion by comparing the results obtained in this study and the experimental results reported in the literature of similar systems show a very good agreement.
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Ez-Zahraouy</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>Laboratoire de Magnétisme et de Physique des Hautes Energies, Departement de Physique, URAC 12 B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Maroc</country><placeName><settlement type="city">Rabat</settlement><region nuts="2">Rabat-Salé-Kénitra</region></placeName></affiliation></author><author><name sortKey="Loulidi, M" sort="Loulidi, M" uniqKey="Loulidi M" first="M." last="Loulidi">M. Loulidi</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>Laboratoire de Magnétisme et de Physique des Hautes Energies, Departement de Physique, URAC 12 B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Maroc</country><placeName><settlement type="city">Rabat</settlement><region nuts="2">Rabat-Salé-Kénitra</region></placeName></affiliation></author><author><name sortKey="Saidi, E H" sort="Saidi, E H" uniqKey="Saidi E" first="E. H." last="Saidi">E. H. Saidi</name><affiliation wicri:level="3"><inist:fA14 i1="02"><s1>Laboratoire de Physique des Hautes Energies, Departement de Physique, B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</s3><sZ>6 aut.</sZ></inist:fA14><country>Maroc</country><placeName><settlement type="city">Rabat</settlement><region nuts="2">Rabat-Salé-Kénitra</region></placeName></affiliation></author><author><name sortKey="Bououdina, M" sort="Bououdina, M" uniqKey="Bououdina M" first="M." last="Bououdina">M. Bououdina</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Nanotechnology Centre, University of Bahrain, P.O. Box 32038</s1><s2>Sukheer</s2><s3>BHR</s3><sZ>7 aut.</sZ></inist:fA14><country>Bahreïn</country><wicri:noRegion>Sukheer</wicri:noRegion></affiliation><affiliation wicri:level="1"><inist:fA14 i1="04"><s1>Department of Physics, College of Science, University of Bahrain, P.O. Box 32038</s1><s2>Sukheer</s2><s3>BHR</s3><sZ>7 aut.</sZ></inist:fA14><country>Bahreïn</country><wicri:noRegion>Sukheer</wicri:noRegion></affiliation></author></titleStmt><publicationStmt><idno type="wicri:source">INIST</idno><idno type="inist">12-0316336</idno><date when="2012">2012</date><idno type="stanalyst">PASCAL 12-0316336 INIST</idno><idno type="RBID">Pascal:12-0316336</idno><idno type="wicri:Area/PascalFrancis/Corpus">000051</idno><idno type="wicri:Area/PascalFrancis/Curation">000244</idno><idno type="wicri:Area/PascalFrancis/Checkpoint">000057</idno><idno type="wicri:explorRef" wicri:stream="PascalFrancis" wicri:step="Checkpoint">000057</idno></publicationStmt><sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">A Comparative First-Principles Study of Fe-, Co-and FeCo-Doped ZnO with Wurtzite and Zinc Blende Structures</title><author><name sortKey="Mamouni, N" sort="Mamouni, N" uniqKey="Mamouni N" first="N." last="Mamouni">N. Mamouni</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>Laboratoire de Magnétisme et de Physique des Hautes Energies, Departement de Physique, URAC 12 B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Maroc</country><placeName><settlement type="city">Rabat</settlement><region nuts="2">Rabat-Salé-Kénitra</region></placeName></affiliation></author><author><name sortKey="Benyoussef, A" sort="Benyoussef, A" uniqKey="Benyoussef A" first="A." last="Benyoussef">A. Benyoussef</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>Laboratoire de Magnétisme et de Physique des Hautes Energies, Departement de Physique, URAC 12 B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Maroc</country><placeName><settlement type="city">Rabat</settlement><region nuts="2">Rabat-Salé-Kénitra</region></placeName></affiliation></author><author><name sortKey="El Kenz, A" sort="El Kenz, A" uniqKey="El Kenz A" first="A." last="El Kenz">A. El Kenz</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>Laboratoire de Magnétisme et de Physique des Hautes Energies, Departement de Physique, URAC 12 B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Maroc</country><placeName><settlement type="city">Rabat</settlement><region nuts="2">Rabat-Salé-Kénitra</region></placeName></affiliation></author><author><name sortKey="Ez Zahraouy, H" sort="Ez Zahraouy, H" uniqKey="Ez Zahraouy H" first="H." last="Ez-Zahraouy">H. Ez-Zahraouy</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>Laboratoire de Magnétisme et de Physique des Hautes Energies, Departement de Physique, URAC 12 B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Maroc</country><placeName><settlement type="city">Rabat</settlement><region nuts="2">Rabat-Salé-Kénitra</region></placeName></affiliation></author><author><name sortKey="Loulidi, M" sort="Loulidi, M" uniqKey="Loulidi M" first="M." last="Loulidi">M. Loulidi</name><affiliation wicri:level="3"><inist:fA14 i1="01"><s1>Laboratoire de Magnétisme et de Physique des Hautes Energies, Departement de Physique, URAC 12 B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</s3><sZ>1 aut.</sZ><sZ>2 aut.</sZ><sZ>3 aut.</sZ><sZ>4 aut.</sZ><sZ>5 aut.</sZ></inist:fA14><country>Maroc</country><placeName><settlement type="city">Rabat</settlement><region nuts="2">Rabat-Salé-Kénitra</region></placeName></affiliation></author><author><name sortKey="Saidi, E H" sort="Saidi, E H" uniqKey="Saidi E" first="E. H." last="Saidi">E. H. Saidi</name><affiliation wicri:level="3"><inist:fA14 i1="02"><s1>Laboratoire de Physique des Hautes Energies, Departement de Physique, B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</s3><sZ>6 aut.</sZ></inist:fA14><country>Maroc</country><placeName><settlement type="city">Rabat</settlement><region nuts="2">Rabat-Salé-Kénitra</region></placeName></affiliation></author><author><name sortKey="Bououdina, M" sort="Bououdina, M" uniqKey="Bououdina M" first="M." last="Bououdina">M. Bououdina</name><affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Nanotechnology Centre, University of Bahrain, P.O. Box 32038</s1><s2>Sukheer</s2><s3>BHR</s3><sZ>7 aut.</sZ></inist:fA14><country>Bahreïn</country><wicri:noRegion>Sukheer</wicri:noRegion></affiliation><affiliation wicri:level="1"><inist:fA14 i1="04"><s1>Department of Physics, College of Science, University of Bahrain, P.O. Box 32038</s1><s2>Sukheer</s2><s3>BHR</s3><sZ>7 aut.</sZ></inist:fA14><country>Bahreïn</country><wicri:noRegion>Sukheer</wicri:noRegion></affiliation></author></analytic><series><title level="j" type="main">Journal of superconductivity and novel magnetism</title><title level="j" type="abbreviated">J. supercond. nov. magn.</title><idno type="ISSN">1557-1939</idno><imprint><date when="2012">2012</date></imprint></series></biblStruct></sourceDesc><seriesStmt><title level="j" type="main">Journal of superconductivity and novel magnetism</title><title level="j" type="abbreviated">J. supercond. nov. magn.</title><idno type="ISSN">1557-1939</idno></seriesStmt></fileDesc><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Ab initio calculations</term><term>Blende structure</term><term>Cobalt additions</term><term>Codoping</term><term>Density functional method</term><term>Diamagnetic materials</term><term>Electronic density of states</term><term>Electronic structure</term><term>Exchange interactions</term><term>Ferromagnetic materials</term><term>Ferromagnetism</term><term>Impurity bands</term><term>Iron additions</term><term>Magnetic moments</term><term>Semimagnetic semiconductors</term><term>Semimetals</term><term>Wurtzite structure</term><term>Zinc oxide</term></keywords><keywords scheme="Pascal" xml:lang="fr"><term>Méthode fonctionnelle densité</term><term>Codopage</term><term>Structure électronique</term><term>Addition fer</term><term>Addition cobalt</term><term>Semimétal</term><term>Densité état électron</term><term>Ferromagnétisme</term><term>Interaction échange</term><term>Calcul ab initio</term><term>Bande impureté</term><term>Moment magnétique</term><term>Semiconducteur semimagnétique</term><term>Oxyde de zinc</term><term>Structure blende</term><term>Structure wurtzite</term><term>Matériau diamagnétique</term><term>Matériau ferromagnétique</term><term>ZnO</term></keywords></textClass></profileDesc></teiHeader><front><div type="abstract" xml:lang="en">First-principles study of the electronic and magnetic properties of zinc-blende and wurtzite structures of Fe-, Co-, and FeCo-doped ZnO is presented. It is found that after doping, this diamagnetic material becomes ferromagnetic and half-metallic. It is also shown that the half-metallicity may be obtained for ZnFeO, ZnCoO, and ZnFe-CoO. The analysis of the spin density reveals that the ferromagnetic phase is due to the ferromagnetic coupling between the p-d states. The effects of Fe on the magnetic properties of ZB and WZ Fe-doped ZnO compound have been investigated with the GGA calculations. In order to understand the role of Fe atom in the ferromagnetism, the density of states both in the presence and absence of Co doping, were calculated. The obtained results show the presence of coupling between Co and Fe atoms through the spin-split impurity band exchange mechanism. More importantly, the calculations show that the magnetic moment changes sensitively with the type of structure of ZnO, zinc-blende, or wurtzite. A discussion by comparing the results obtained in this study and the experimental results reported in the literature of similar systems show a very good agreement.</div></front></TEI><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>1557-1939</s0></fA01><fA03 i2="1"><s0>J. supercond. nov. magn.</s0></fA03><fA05><s2>25</s2></fA05><fA06><s2>5</s2></fA06><fA08 i1="01" i2="1" l="ENG"><s1>A Comparative First-Principles Study of Fe-, Co-and FeCo-Doped ZnO with Wurtzite and Zinc Blende Structures</s1></fA08><fA11 i1="01" i2="1"><s1>MAMOUNI (N.)</s1></fA11><fA11 i1="02" i2="1"><s1>BENYOUSSEF (A.)</s1></fA11><fA11 i1="03" i2="1"><s1>EL KENZ (A.)</s1></fA11><fA11 i1="04" i2="1"><s1>EZ-ZAHRAOUY (H.)</s1></fA11><fA11 i1="05" i2="1"><s1>LOULIDI (M.)</s1></fA11><fA11 i1="06" i2="1"><s1>SAIDI (E. H.)</s1></fA11><fA11 i1="07" i2="1"><s1>BOUOUDINA (M.)</s1></fA11><fA14 i1="01"><s1>Laboratoire de Magnétisme et de Physique des Hautes Energies, Departement de Physique, URAC 12 B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</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>Laboratoire de Physique des Hautes Energies, Departement de Physique, B.P. 1014, Faculté des Sciences</s1><s2>Rabat</s2><s3>MAR</s3><sZ>6 aut.</sZ></fA14><fA14 i1="03"><s1>Nanotechnology Centre, University of Bahrain, P.O. Box 32038</s1><s2>Sukheer</s2><s3>BHR</s3><sZ>7 aut.</sZ></fA14><fA14 i1="04"><s1>Department of Physics, College of Science, University of Bahrain, P.O. Box 32038</s1><s2>Sukheer</s2><s3>BHR</s3><sZ>7 aut.</sZ></fA14><fA20><s1>1579-1587</s1></fA20><fA21><s1>2012</s1></fA21><fA23 i1="01"><s0>ENG</s0></fA23><fA43 i1="01"><s1>INIST</s1><s2>21987</s2><s5>354000506621630600</s5></fA43><fA44><s0>0000</s0><s1>© 2012 INIST-CNRS. All rights reserved.</s1></fA44><fA45><s0>28 ref.</s0></fA45><fA47 i1="01" i2="1"><s0>12-0316336</s0></fA47><fA60><s1>P</s1></fA60><fA61><s0>A</s0></fA61><fA64 i1="01" i2="1"><s0>Journal of superconductivity and novel magnetism</s0></fA64><fA66 i1="01"><s0>USA</s0></fA66><fC01 i1="01" l="ENG"><s0>First-principles study of the electronic and magnetic properties of zinc-blende and wurtzite structures of Fe-, Co-, and FeCo-doped ZnO is presented. It is found that after doping, this diamagnetic material becomes ferromagnetic and half-metallic. It is also shown that the half-metallicity may be obtained for ZnFeO, ZnCoO, and ZnFe-CoO. The analysis of the spin density reveals that the ferromagnetic phase is due to the ferromagnetic coupling between the p-d states. The effects of Fe on the magnetic properties of ZB and WZ Fe-doped ZnO compound have been investigated with the GGA calculations. In order to understand the role of Fe atom in the ferromagnetism, the density of states both in the presence and absence of Co doping, were calculated. The obtained results show the presence of coupling between Co and Fe atoms through the spin-split impurity band exchange mechanism. More importantly, the calculations show that the magnetic moment changes sensitively with the type of structure of ZnO, zinc-blende, or wurtzite. A discussion by comparing the results obtained in this study and the experimental results reported in the literature of similar systems show a very good agreement.</s0></fC01><fC02 i1="01" i2="3"><s0>001B70A20N</s0></fC02><fC02 i1="02" i2="3"><s0>001B70E50P</s0></fC02><fC03 i1="01" i2="3" l="FRE"><s0>Méthode fonctionnelle densité</s0><s5>02</s5></fC03><fC03 i1="01" i2="3" l="ENG"><s0>Density functional method</s0><s5>02</s5></fC03><fC03 i1="02" i2="X" l="FRE"><s0>Codopage</s0><s5>03</s5></fC03><fC03 i1="02" i2="X" l="ENG"><s0>Codoping</s0><s5>03</s5></fC03><fC03 i1="02" i2="X" l="SPA"><s0>Codrogado</s0><s5>03</s5></fC03><fC03 i1="03" i2="3" l="FRE"><s0>Structure électronique</s0><s5>04</s5></fC03><fC03 i1="03" i2="3" l="ENG"><s0>Electronic structure</s0><s5>04</s5></fC03><fC03 i1="04" i2="3" l="FRE"><s0>Addition fer</s0><s5>05</s5></fC03><fC03 i1="04" i2="3" l="ENG"><s0>Iron additions</s0><s5>05</s5></fC03><fC03 i1="05" i2="3" l="FRE"><s0>Addition cobalt</s0><s5>06</s5></fC03><fC03 i1="05" i2="3" l="ENG"><s0>Cobalt additions</s0><s5>06</s5></fC03><fC03 i1="06" i2="3" l="FRE"><s0>Semimétal</s0><s5>07</s5></fC03><fC03 i1="06" i2="3" l="ENG"><s0>Semimetals</s0><s5>07</s5></fC03><fC03 i1="07" i2="3" l="FRE"><s0>Densité état électron</s0><s5>08</s5></fC03><fC03 i1="07" i2="3" l="ENG"><s0>Electronic density of states</s0><s5>08</s5></fC03><fC03 i1="08" i2="3" l="FRE"><s0>Ferromagnétisme</s0><s5>09</s5></fC03><fC03 i1="08" i2="3" l="ENG"><s0>Ferromagnetism</s0><s5>09</s5></fC03><fC03 i1="09" i2="3" l="FRE"><s0>Interaction échange</s0><s5>10</s5></fC03><fC03 i1="09" i2="3" l="ENG"><s0>Exchange interactions</s0><s5>10</s5></fC03><fC03 i1="10" i2="3" l="FRE"><s0>Calcul ab initio</s0><s5>11</s5></fC03><fC03 i1="10" i2="3" l="ENG"><s0>Ab initio calculations</s0><s5>11</s5></fC03><fC03 i1="11" i2="3" l="FRE"><s0>Bande impureté</s0><s5>12</s5></fC03><fC03 i1="11" i2="3" l="ENG"><s0>Impurity bands</s0><s5>12</s5></fC03><fC03 i1="12" i2="3" l="FRE"><s0>Moment magnétique</s0><s5>13</s5></fC03><fC03 i1="12" i2="3" l="ENG"><s0>Magnetic moments</s0><s5>13</s5></fC03><fC03 i1="13" i2="3" l="FRE"><s0>Semiconducteur semimagnétique</s0><s5>15</s5></fC03><fC03 i1="13" i2="3" l="ENG"><s0>Semimagnetic semiconductors</s0><s5>15</s5></fC03><fC03 i1="14" i2="X" l="FRE"><s0>Oxyde de zinc</s0><s5>16</s5></fC03><fC03 i1="14" i2="X" l="ENG"><s0>Zinc oxide</s0><s5>16</s5></fC03><fC03 i1="14" i2="X" l="SPA"><s0>Zinc óxido</s0><s5>16</s5></fC03><fC03 i1="15" i2="X" l="FRE"><s0>Structure blende</s0><s5>17</s5></fC03><fC03 i1="15" i2="X" l="ENG"><s0>Blende structure</s0><s5>17</s5></fC03><fC03 i1="15" i2="X" l="SPA"><s0>Estructura blenda</s0><s5>17</s5></fC03><fC03 i1="16" i2="X" l="FRE"><s0>Structure wurtzite</s0><s5>18</s5></fC03><fC03 i1="16" i2="X" l="ENG"><s0>Wurtzite structure</s0><s5>18</s5></fC03><fC03 i1="16" i2="X" l="SPA"><s0>Estructura wurtzita</s0><s5>18</s5></fC03><fC03 i1="17" i2="3" l="FRE"><s0>Matériau diamagnétique</s0><s5>19</s5></fC03><fC03 i1="17" i2="3" l="ENG"><s0>Diamagnetic materials</s0><s5>19</s5></fC03><fC03 i1="18" i2="3" l="FRE"><s0>Matériau ferromagnétique</s0><s5>20</s5></fC03><fC03 i1="18" i2="3" l="ENG"><s0>Ferromagnetic materials</s0><s5>20</s5></fC03><fC03 i1="19" i2="3" l="FRE"><s0>ZnO</s0><s4>INC</s4><s5>52</s5></fC03><fN21><s1>240</s1></fN21></pA></standard></inist><affiliations><list><country><li>Bahreïn</li><li>Maroc</li></country><region><li>Rabat-Salé-Kénitra</li></region><settlement><li>Rabat</li></settlement></list><tree><country name="Maroc"><region name="Rabat-Salé-Kénitra"><name sortKey="Mamouni, N" sort="Mamouni, N" uniqKey="Mamouni N" first="N." last="Mamouni">N. Mamouni</name></region><name sortKey="Benyoussef, A" sort="Benyoussef, A" uniqKey="Benyoussef A" first="A." last="Benyoussef">A. Benyoussef</name><name sortKey="El Kenz, A" sort="El Kenz, A" uniqKey="El Kenz A" first="A." last="El Kenz">A. El Kenz</name><name sortKey="Ez Zahraouy, H" sort="Ez Zahraouy, H" uniqKey="Ez Zahraouy H" first="H." last="Ez-Zahraouy">H. Ez-Zahraouy</name><name sortKey="Loulidi, M" sort="Loulidi, M" uniqKey="Loulidi M" first="M." last="Loulidi">M. Loulidi</name><name sortKey="Saidi, E H" sort="Saidi, E H" uniqKey="Saidi E" first="E. H." last="Saidi">E. H. Saidi</name></country><country name="Bahreïn"><noRegion><name sortKey="Bououdina, M" sort="Bououdina, M" uniqKey="Bououdina M" first="M." last="Bououdina">M. Bououdina</name></noRegion><name sortKey="Bououdina, M" sort="Bououdina, M" uniqKey="Bououdina M" first="M." last="Bououdina">M. Bououdina</name></country></tree></affiliations></record>Pour manipuler ce document sous Unix (Dilib)
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