CobaltMaghrebV1, PascalFrancis, Curation, bibRecord, 000248

Ab-initio Calculation of Half-Metal Ferrimagnetic Sn0.9Mn0.05Co0.05O2

Identifieur interne : 000248 ( PascalFrancis/Curation ); précédent : 000247; suivant : 000249

Ab-initio Calculation of Half-Metal Ferrimagnetic Sn0.9Mn0.05Co0.05O2

Auteurs : O. Mounkachi [Maroc] ; E. Salmani [Maroc] ; H. El Moussaoui [Maroc] ; M. Hamedoun [Maroc] ; H. Ez-Zahraouy [Maroc] ; A. Benyoussef [Maroc]

Source :

Journal of superconductivity and novel magnetism [ 1557-1939 ] ; 2012.

RBID : Pascal:12-0349377

Descripteurs français

Pascal (Inist)
- Etude théorique, Calcul ab initio, Semimétal, Densité spin, Méthode fonctionnelle densité, Calcul KKR, Calcul CPA, Composé minéral, Matériau dopé, Codopage, Matériau ferrimagnétique, Oxyde d'étain, Addition manganèse, Impureté magnétique, Addition cobalt, Approximation densité locale, Hybridation, Structure bande, Théorie bandes, SnO2, 7115M, 7550P.
Wicri :
- topic : Composé minéral.

English descriptors

KwdEn :
- Ab initio calculations, Band structure, Band theory, CPA calculations, Cobalt additions, Codoping, Density functional method, Doped materials, Ferrimagnetic materials, Hybridization, Inorganic compounds, KKR calculations, Local density approximation, Magnetic impurities, Manganese additions, Semimetals, Spin density, Theoretical study, Tin oxide.

Abstract

Based on first-principles spin-density functional calculations, using the Korringa-Kohn-Rostoker (KKR) method combined with the coherent potential approximation (CPA), we investigated the half-metallic ferrimagnetic properties of SnO₂ codoped with Mn and Co impurities (Sn_0.90(Mn_0.05, Co_0.05)O₂) within the self-interaction-corrected (SIC) local density approximation. Mechanism of hybridization and interaction between magnetic ions in Sn_0.90(Mn_0.05, Co_0.05)O₂ is investigated. The band structure model has been used to explain the strong ferrimagnetic interaction observed and the mechanism that stabilizes this state is proposed.

A01	`01`	`1`		`@0 1557-1939`
A03		`1`		`@0 J. supercond. nov. magn.`
A05				`@2 25`
A06				`@2 6`
A08	`01`	`1`	`ENG`	`@1 Ab-initio Calculation of Half-Metal Ferrimagnetic Sn_0.9Mn_0.05Co_0.05O₂`
A11	`01`	`1`		`@1 MOUNKACHI (O.)`
A11	`02`	`1`		`@1 SALMANI (E.)`
A11	`03`	`1`		`@1 EL MOUSSAOUI (H.)`
A11	`04`	`1`		`@1 HAMEDOUN (M.)`
A11	`05`	`1`		`@1 EZ-ZAHRAOUY (H.)`
A11	`06`	`1`		`@1 BENYOUSSEF (A.)`
A14	`01`			`@1 Institute of Nanomaterials and Nanotechnology, MAScIR @2 Rabat @3 MAR @Z 1 aut. @Z 3 aut. @Z 4 aut. @Z 6 aut.`
A14	`02`			`@1 LMPHE, associe au CNRST (URAC 12), Faculté des Sciences, Universite Mohammed V-Agdal @2 Rabat @3 MAR @Z 2 aut. @Z 3 aut. @Z 5 aut. @Z 6 aut.`
A14	`03`			`@1 Hassan II Academy of Science and Technology @2 Rabat @3 MAR @Z 6 aut.`
A20				`@1 2069-2074`
A21				`@1 2012`
A23	`01`			`@0 ENG`
A43	`01`			`@1 INIST @2 21987 @5 354000508333350660`
A44				`@0 0000 @1 © 2012 INIST-CNRS. All rights reserved.`
A45				`@0 33 ref.`
A47	`01`	`1`		`@0 12-0349377`
A60				`@1 P`
A61				`@0 A`
A64	`01`	`1`		`@0 Journal of superconductivity and novel magnetism`
A66	`01`			`@0 USA`
C01	`01`		`ENG`	@0 Based on first-principles spin-density functional calculations, using the Korringa-Kohn-Rostoker (KKR) method combined with the coherent potential approximation (CPA), we investigated the half-metallic ferrimagnetic properties of SnO₂ codoped with Mn and Co impurities (Sn_0.90(Mn_0.05, Co_0.05)O₂) within the self-interaction-corrected (SIC) local density approximation. Mechanism of hybridization and interaction between magnetic ions in Sn_0.90(Mn_0.05, Co_0.05)O₂ is investigated. The band structure model has been used to explain the strong ferrimagnetic interaction observed and the mechanism that stabilizes this state is proposed.
C02	`01`	`3`		`@0 001B70A15`
C02	`02`	`3`		`@0 001B70E50P`
C03	`01`	`3`	`FRE`	`@0 Etude théorique @5 21`
C03	`01`	`3`	`ENG`	`@0 Theoretical study @5 21`
C03	`02`	`3`	`FRE`	`@0 Calcul ab initio @5 41`
C03	`02`	`3`	`ENG`	`@0 Ab initio calculations @5 41`
C03	`03`	`3`	`FRE`	`@0 Semimétal @5 42`
C03	`03`	`3`	`ENG`	`@0 Semimetals @5 42`
C03	`04`	`3`	`FRE`	`@0 Densité spin @5 43`
C03	`04`	`3`	`ENG`	`@0 Spin density @5 43`
C03	`05`	`3`	`FRE`	`@0 Méthode fonctionnelle densité @5 44`
C03	`05`	`3`	`ENG`	`@0 Density functional method @5 44`
C03	`06`	`3`	`FRE`	`@0 Calcul KKR @5 45`
C03	`06`	`3`	`ENG`	`@0 KKR calculations @5 45`
C03	`07`	`3`	`FRE`	`@0 Calcul CPA @5 46`
C03	`07`	`3`	`ENG`	`@0 CPA calculations @5 46`
C03	`08`	`3`	`FRE`	`@0 Composé minéral @5 50`
C03	`08`	`3`	`ENG`	`@0 Inorganic compounds @5 50`
C03	`09`	`3`	`FRE`	`@0 Matériau dopé @5 51`
C03	`09`	`3`	`ENG`	`@0 Doped materials @5 51`
C03	`10`	`X`	`FRE`	`@0 Codopage @5 57`
C03	`10`	`X`	`ENG`	`@0 Codoping @5 57`
C03	`10`	`X`	`SPA`	`@0 Codrogado @5 57`
C03	`11`	`3`	`FRE`	`@0 Matériau ferrimagnétique @5 61`
C03	`11`	`3`	`ENG`	`@0 Ferrimagnetic materials @5 61`
C03	`12`	`X`	`FRE`	`@0 Oxyde d'étain @5 62`
C03	`12`	`X`	`ENG`	`@0 Tin oxide @5 62`
C03	`12`	`X`	`SPA`	`@0 Estaño óxido @5 62`
C03	`13`	`3`	`FRE`	`@0 Addition manganèse @5 63`
C03	`13`	`3`	`ENG`	`@0 Manganese additions @5 63`
C03	`14`	`3`	`FRE`	`@0 Impureté magnétique @5 64`
C03	`14`	`3`	`ENG`	`@0 Magnetic impurities @5 64`
C03	`15`	`3`	`FRE`	`@0 Addition cobalt @5 65`
C03	`15`	`3`	`ENG`	`@0 Cobalt additions @5 65`
C03	`16`	`X`	`FRE`	`@0 Approximation densité locale @5 66`
C03	`16`	`X`	`ENG`	`@0 Local density approximation @5 66`
C03	`16`	`X`	`SPA`	`@0 Aproximación densidad local @5 66`
C03	`17`	`3`	`FRE`	`@0 Hybridation @5 67`
C03	`17`	`3`	`ENG`	`@0 Hybridization @5 67`
C03	`18`	`3`	`FRE`	`@0 Structure bande @5 68`
C03	`18`	`3`	`ENG`	`@0 Band structure @5 68`
C03	`19`	`3`	`FRE`	`@0 Théorie bandes @5 69`
C03	`19`	`3`	`ENG`	`@0 Band theory @5 69`
C03	`20`	`3`	`FRE`	`@0 SnO2 @4 INC @5 83`
C03	`21`	`3`	`FRE`	`@0 7115M @4 INC @5 84`
C03	`22`	`3`	`FRE`	`@0 7550P @4 INC @5 92`
N21				`@1 268`

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Le document en format XML

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Mn<sub>0.05</sub>
Co<sub>0.05</sub>
O<sub>2</sub>
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<sourceDesc><biblStruct><analytic><title xml:lang="en" level="a">Ab-initio Calculation of Half-Metal Ferrimagnetic Sn<sub>0.9</sub>
Mn<sub>0.05</sub>
Co<sub>0.05</sub>
O<sub>2</sub>
</title>
<author><name sortKey="Mounkachi, O" sort="Mounkachi, O" uniqKey="Mounkachi O" first="O." last="Mounkachi">O. Mounkachi</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Institute of Nanomaterials and Nanotechnology, MAScIR</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
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</affiliation>
</author>
<author><name sortKey="Salmani, E" sort="Salmani, E" uniqKey="Salmani E" first="E." last="Salmani">E. Salmani</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>LMPHE, associe au CNRST (URAC 12), Faculté des Sciences, Universite Mohammed V-Agdal</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
</author>
<author><name sortKey="El Moussaoui, H" sort="El Moussaoui, H" uniqKey="El Moussaoui H" first="H." last="El Moussaoui">H. El Moussaoui</name>
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<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
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<sZ>3 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
</author>
<author><name sortKey="Hamedoun, M" sort="Hamedoun, M" uniqKey="Hamedoun M" first="M." last="Hamedoun">M. Hamedoun</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Institute of Nanomaterials and Nanotechnology, MAScIR</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
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<sZ>4 aut.</sZ>
<sZ>6 aut.</sZ>
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</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="1"><inist:fA14 i1="02"><s1>LMPHE, associe au CNRST (URAC 12), Faculté des Sciences, Universite Mohammed V-Agdal</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
</author>
<author><name sortKey="Benyoussef, A" sort="Benyoussef, A" uniqKey="Benyoussef A" first="A." last="Benyoussef">A. Benyoussef</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Institute of Nanomaterials and Nanotechnology, MAScIR</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>LMPHE, associe au CNRST (URAC 12), Faculté des Sciences, Universite Mohammed V-Agdal</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</affiliation>
<affiliation wicri:level="1"><inist:fA14 i1="03"><s1>Hassan II Academy of Science and Technology</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
<sZ>6 aut.</sZ>
</inist:fA14>
<country>Maroc</country>
</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>
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<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>Band structure</term>
<term>Band theory</term>
<term>CPA calculations</term>
<term>Cobalt additions</term>
<term>Codoping</term>
<term>Density functional method</term>
<term>Doped materials</term>
<term>Ferrimagnetic materials</term>
<term>Hybridization</term>
<term>Inorganic compounds</term>
<term>KKR calculations</term>
<term>Local density approximation</term>
<term>Magnetic impurities</term>
<term>Manganese additions</term>
<term>Semimetals</term>
<term>Spin density</term>
<term>Theoretical study</term>
<term>Tin oxide</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Etude théorique</term>
<term>Calcul ab initio</term>
<term>Semimétal</term>
<term>Densité spin</term>
<term>Méthode fonctionnelle densité</term>
<term>Calcul KKR</term>
<term>Calcul CPA</term>
<term>Composé minéral</term>
<term>Matériau dopé</term>
<term>Codopage</term>
<term>Matériau ferrimagnétique</term>
<term>Oxyde d'étain</term>
<term>Addition manganèse</term>
<term>Impureté magnétique</term>
<term>Addition cobalt</term>
<term>Approximation densité locale</term>
<term>Hybridation</term>
<term>Structure bande</term>
<term>Théorie bandes</term>
<term>SnO2</term>
<term>7115M</term>
<term>7550P</term>
</keywords>
<keywords scheme="Wicri" type="topic" xml:lang="fr"><term>Composé minéral</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front><div type="abstract" xml:lang="en">Based on first-principles spin-density functional calculations, using the Korringa-Kohn-Rostoker (KKR) method combined with the coherent potential approximation (CPA), we investigated the half-metallic ferrimagnetic properties of SnO<sub>2</sub>
 codoped with Mn and Co impurities (Sn<sub>0.90</sub>
(Mn<sub>0.05</sub>
, Co<sub>0.05</sub>
)O<sub>2</sub>
) within the self-interaction-corrected (SIC) local density approximation. Mechanism of hybridization and interaction between magnetic ions in Sn<sub>0.90</sub>
(Mn<sub>0.05</sub>
, Co<sub>0.05</sub>
)O<sub>2</sub>
 is investigated. The band structure model has been used to explain the strong ferrimagnetic interaction observed and the mechanism that stabilizes this state is proposed.</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>6</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG"><s1>Ab-initio Calculation of Half-Metal Ferrimagnetic Sn<sub>0.9</sub>
Mn<sub>0.05</sub>
Co<sub>0.05</sub>
O<sub>2</sub>
</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>MOUNKACHI (O.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>SALMANI (E.)</s1>
</fA11>
<fA11 i1="03" i2="1"><s1>EL MOUSSAOUI (H.)</s1>
</fA11>
<fA11 i1="04" i2="1"><s1>HAMEDOUN (M.)</s1>
</fA11>
<fA11 i1="05" i2="1"><s1>EZ-ZAHRAOUY (H.)</s1>
</fA11>
<fA11 i1="06" i2="1"><s1>BENYOUSSEF (A.)</s1>
</fA11>
<fA14 i1="01"><s1>Institute of Nanomaterials and Nanotechnology, MAScIR</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>6 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>LMPHE, associe au CNRST (URAC 12), Faculté des Sciences, Universite Mohammed V-Agdal</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>5 aut.</sZ>
<sZ>6 aut.</sZ>
</fA14>
<fA14 i1="03"><s1>Hassan II Academy of Science and Technology</s1>
<s2>Rabat</s2>
<s3>MAR</s3>
<sZ>6 aut.</sZ>
</fA14>
<fA20><s1>2069-2074</s1>
</fA20>
<fA21><s1>2012</s1>
</fA21>
<fA23 i1="01"><s0>ENG</s0>
</fA23>
<fA43 i1="01"><s1>INIST</s1>
<s2>21987</s2>
<s5>354000508333350660</s5>
</fA43>
<fA44><s0>0000</s0>
<s1>© 2012 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45><s0>33 ref.</s0>
</fA45>
<fA47 i1="01" i2="1"><s0>12-0349377</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>Based on first-principles spin-density functional calculations, using the Korringa-Kohn-Rostoker (KKR) method combined with the coherent potential approximation (CPA), we investigated the half-metallic ferrimagnetic properties of SnO<sub>2</sub>
 codoped with Mn and Co impurities (Sn<sub>0.90</sub>
(Mn<sub>0.05</sub>
, Co<sub>0.05</sub>
)O<sub>2</sub>
) within the self-interaction-corrected (SIC) local density approximation. Mechanism of hybridization and interaction between magnetic ions in Sn<sub>0.90</sub>
(Mn<sub>0.05</sub>
, Co<sub>0.05</sub>
)O<sub>2</sub>
 is investigated. The band structure model has been used to explain the strong ferrimagnetic interaction observed and the mechanism that stabilizes this state is proposed.</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70A15</s0>
</fC02>
<fC02 i1="02" i2="3"><s0>001B70E50P</s0>
</fC02>
<fC03 i1="01" i2="3" l="FRE"><s0>Etude théorique</s0>
<s5>21</s5>
</fC03>
<fC03 i1="01" i2="3" l="ENG"><s0>Theoretical study</s0>
<s5>21</s5>
</fC03>
<fC03 i1="02" i2="3" l="FRE"><s0>Calcul ab initio</s0>
<s5>41</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Ab initio calculations</s0>
<s5>41</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Semimétal</s0>
<s5>42</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Semimetals</s0>
<s5>42</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Densité spin</s0>
<s5>43</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Spin density</s0>
<s5>43</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Méthode fonctionnelle densité</s0>
<s5>44</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Density functional method</s0>
<s5>44</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE"><s0>Calcul KKR</s0>
<s5>45</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG"><s0>KKR calculations</s0>
<s5>45</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Calcul CPA</s0>
<s5>46</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>CPA calculations</s0>
<s5>46</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Composé minéral</s0>
<s5>50</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Inorganic compounds</s0>
<s5>50</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Matériau dopé</s0>
<s5>51</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Doped materials</s0>
<s5>51</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE"><s0>Codopage</s0>
<s5>57</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG"><s0>Codoping</s0>
<s5>57</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA"><s0>Codrogado</s0>
<s5>57</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE"><s0>Matériau ferrimagnétique</s0>
<s5>61</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG"><s0>Ferrimagnetic materials</s0>
<s5>61</s5>
</fC03>
<fC03 i1="12" i2="X" l="FRE"><s0>Oxyde d'étain</s0>
<s5>62</s5>
</fC03>
<fC03 i1="12" i2="X" l="ENG"><s0>Tin oxide</s0>
<s5>62</s5>
</fC03>
<fC03 i1="12" i2="X" l="SPA"><s0>Estaño óxido</s0>
<s5>62</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE"><s0>Addition manganèse</s0>
<s5>63</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG"><s0>Manganese additions</s0>
<s5>63</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>Impureté magnétique</s0>
<s5>64</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG"><s0>Magnetic impurities</s0>
<s5>64</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>Addition cobalt</s0>
<s5>65</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG"><s0>Cobalt additions</s0>
<s5>65</s5>
</fC03>
<fC03 i1="16" i2="X" l="FRE"><s0>Approximation densité locale</s0>
<s5>66</s5>
</fC03>
<fC03 i1="16" i2="X" l="ENG"><s0>Local density approximation</s0>
<s5>66</s5>
</fC03>
<fC03 i1="16" i2="X" l="SPA"><s0>Aproximación densidad local</s0>
<s5>66</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>Hybridation</s0>
<s5>67</s5>
</fC03>
<fC03 i1="17" i2="3" l="ENG"><s0>Hybridization</s0>
<s5>67</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>Structure bande</s0>
<s5>68</s5>
</fC03>
<fC03 i1="18" i2="3" l="ENG"><s0>Band structure</s0>
<s5>68</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>Théorie bandes</s0>
<s5>69</s5>
</fC03>
<fC03 i1="19" i2="3" l="ENG"><s0>Band theory</s0>
<s5>69</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>SnO2</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03>
<fC03 i1="21" i2="3" l="FRE"><s0>7115M</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03>
<fC03 i1="22" i2="3" l="FRE"><s0>7550P</s0>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fN21><s1>268</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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Ab-initio Calculation of Half-Metal Ferrimagnetic Sn0.9Mn0.05Co0.05O2

Ab-initio Calculation of Half-Metal Ferrimagnetic Sn0.9Mn0.05Co0.05O2

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