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Electronic structure, Fermi surface topology and spectroscopic optical properties of LaBaCo2O5.5 compound

Identifieur interne : 000285 ( PascalFrancis/Curation ); précédent : 000284; suivant : 000286

Electronic structure, Fermi surface topology and spectroscopic optical properties of LaBaCo2O5.5 compound

Auteurs : A. H. Reshak [République tchèque, Malaisie] ; Y. Al-Douri [Malaisie] ; R. Khenata [Algérie] ; Wilayat Khan [République tchèque] ; SALEEM AYAZ KHAN [République tchèque] ; Sikander Azam [République tchèque]

Source :

RBID : Pascal:14-0154311

Descripteurs français

English descriptors

Abstract

We have investigated the electronic band structure, Fermi surface topology, chemical bonding and optical properties of LaBaCo2O5.5 compound. The first-principle calculations based on density functional theory (DFT) by means of the full-potential linearized augmented plane-wave method were employed. The atomic positions of LaBaCo2O5.5 compound were optimized by minimizing the forces acting on atoms. We employed the local density approximation (LDA), generalized gradient approximation (GGA) and Engel-Vosko GGA (EVGGA) to treat the exchange correlation potential by solving Kohn-Sham equations. Electronic structure and bonding properties are studied throughout the calculation of densities of states, Fermi surfaces and charge densities. Furthermore, the optical properties are investigated via the calculation of the dielectric tensor component in order to characterize the linear optical properties. Optical spectra are analyzed by means of the electronic structure, which provides theoretical understanding of the conduction mechanism of the investigated compound.
pA  
A01 01  1    @0 0304-8853
A02 01      @0 JMMMDC
A03   1    @0 J. magn. magn. mater.
A05       @2 363
A08 01  1  ENG  @1 Electronic structure, Fermi surface topology and spectroscopic optical properties of LaBaCo2O5.5 compound
A11 01  1    @1 RESHAK (A. H.)
A11 02  1    @1 AL-DOURI (Y.)
A11 03  1    @1 KHENATA (R.)
A11 04  1    @1 KHAN (Wilayat)
A11 05  1    @1 SALEEM AYAZ KHAN
A11 06  1    @1 AZAM (Sikander)
A14 01      @1 New Technologies - Research Center, University of West Bohemia, Univerzitni 8 @2 Pilsen 306 14 @3 CZE @Z 1 aut. @Z 4 aut. @Z 5 aut. @Z 6 aut.
A14 02      @1 Center of Excellence Geopolymer and Green Technology, School of Material Engineering, University Malaysia Perlis @2 01007 Kangar, Perlis @3 MYS @Z 1 aut.
A14 03      @1 Institute of Nano Electronic Engineering, University Malaysia Perlis @2 01000 Kangar, Perlis @3 MYS @Z 2 aut.
A14 04      @1 Laboratoire de Physique Quantique et de Modélisation Mathématique (LPQ3M), Département de Technologie, Université de Mascara @2 Mascara 29000 @3 DZA @Z 3 aut.
A20       @1 133-139
A21       @1 2014
A23 01      @0 ENG
A43 01      @1 INIST @2 17230 @5 354000508241280220
A44       @0 0000 @1 © 2014 INIST-CNRS. All rights reserved.
A45       @0 46 ref.
A47 01  1    @0 14-0154311
A60       @1 P
A61       @0 A
A64 01  1    @0 Journal of magnetism and magnetic materials
A66 01      @0 NLD
C01 01    ENG  @0 We have investigated the electronic band structure, Fermi surface topology, chemical bonding and optical properties of LaBaCo2O5.5 compound. The first-principle calculations based on density functional theory (DFT) by means of the full-potential linearized augmented plane-wave method were employed. The atomic positions of LaBaCo2O5.5 compound were optimized by minimizing the forces acting on atoms. We employed the local density approximation (LDA), generalized gradient approximation (GGA) and Engel-Vosko GGA (EVGGA) to treat the exchange correlation potential by solving Kohn-Sham equations. Electronic structure and bonding properties are studied throughout the calculation of densities of states, Fermi surfaces and charge densities. Furthermore, the optical properties are investigated via the calculation of the dielectric tensor component in order to characterize the linear optical properties. Optical spectra are analyzed by means of the electronic structure, which provides theoretical understanding of the conduction mechanism of the investigated compound.
C02 01  3    @0 001B70H20B
C02 02  3    @0 001B70A18
C03 01  3  FRE  @0 Densité état électron @5 02
C03 01  3  ENG  @0 Electronic density of states @5 02
C03 02  3  FRE  @0 Fonction diélectrique @5 03
C03 02  3  ENG  @0 Dielectric function @5 03
C03 03  3  FRE  @0 Surface Fermi @5 04
C03 03  3  ENG  @0 Fermi surface @5 04
C03 04  3  FRE  @0 Structure bande @5 06
C03 04  3  ENG  @0 Band structure @5 06
C03 05  3  FRE  @0 Liaison chimique @5 07
C03 05  3  ENG  @0 Chemical bonds @5 07
C03 06  3  FRE  @0 Méthode fonctionnelle densité @5 08
C03 06  3  ENG  @0 Density functional method @5 08
C03 07  3  FRE  @0 Calcul APW @5 09
C03 07  3  ENG  @0 APW calculations @5 09
C03 08  X  FRE  @0 Position atomique @5 10
C03 08  X  ENG  @0 Atomic position @5 10
C03 08  X  SPA  @0 Posición atómica @5 10
C03 09  X  FRE  @0 Baryum Lanthane Cobalt Oxyde Mixte @2 NC @2 NA @5 11
C03 09  X  ENG  @0 Barium Lanthanum Cobalt Oxides Mixed @2 NC @2 NA @5 11
C03 09  X  SPA  @0 Mixto @2 NC @2 NA @5 11
C03 10  X  FRE  @0 Approximation densité locale @5 12
C03 10  X  ENG  @0 Local density approximation @5 12
C03 10  X  SPA  @0 Aproximación densidad local @5 12
C03 11  3  FRE  @0 Approximation gradient généralisé @5 13
C03 11  3  ENG  @0 Generalized gradient approximation @5 13
N21       @1 195

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Pascal:14-0154311

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<term>Barium Lanthanum Cobalt Oxides Mixed</term>
<term>Chemical bonds</term>
<term>Density functional method</term>
<term>Dielectric function</term>
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<term>Calcul APW</term>
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<div type="abstract" xml:lang="en">We have investigated the electronic band structure, Fermi surface topology, chemical bonding and optical properties of LaBaCo
<sub>2</sub>
O
<sub>5.5</sub>
compound. The first-principle calculations based on density functional theory (DFT) by means of the full-potential linearized augmented plane-wave method were employed. The atomic positions of LaBaCo
<sub>2</sub>
O
<sub>5.5</sub>
compound were optimized by minimizing the forces acting on atoms. We employed the local density approximation (LDA), generalized gradient approximation (GGA) and Engel-Vosko GGA (EVGGA) to treat the exchange correlation potential by solving Kohn-Sham equations. Electronic structure and bonding properties are studied throughout the calculation of densities of states, Fermi surfaces and charge densities. Furthermore, the optical properties are investigated via the calculation of the dielectric tensor component in order to characterize the linear optical properties. Optical spectra are analyzed by means of the electronic structure, which provides theoretical understanding of the conduction mechanism of the investigated compound.</div>
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O
<sub>5.5</sub>
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<s0>We have investigated the electronic band structure, Fermi surface topology, chemical bonding and optical properties of LaBaCo
<sub>2</sub>
O
<sub>5.5</sub>
compound. The first-principle calculations based on density functional theory (DFT) by means of the full-potential linearized augmented plane-wave method were employed. The atomic positions of LaBaCo
<sub>2</sub>
O
<sub>5.5</sub>
compound were optimized by minimizing the forces acting on atoms. We employed the local density approximation (LDA), generalized gradient approximation (GGA) and Engel-Vosko GGA (EVGGA) to treat the exchange correlation potential by solving Kohn-Sham equations. Electronic structure and bonding properties are studied throughout the calculation of densities of states, Fermi surfaces and charge densities. Furthermore, the optical properties are investigated via the calculation of the dielectric tensor component in order to characterize the linear optical properties. Optical spectra are analyzed by means of the electronic structure, which provides theoretical understanding of the conduction mechanism of the investigated compound.</s0>
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<s5>04</s5>
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<s5>04</s5>
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<s0>Structure bande</s0>
<s5>06</s5>
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<s5>06</s5>
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<s5>07</s5>
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<s5>08</s5>
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<s5>08</s5>
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<fC03 i1="07" i2="3" l="FRE">
<s0>Calcul APW</s0>
<s5>09</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>APW calculations</s0>
<s5>09</s5>
</fC03>
<fC03 i1="08" i2="X" l="FRE">
<s0>Position atomique</s0>
<s5>10</s5>
</fC03>
<fC03 i1="08" i2="X" l="ENG">
<s0>Atomic position</s0>
<s5>10</s5>
</fC03>
<fC03 i1="08" i2="X" l="SPA">
<s0>Posición atómica</s0>
<s5>10</s5>
</fC03>
<fC03 i1="09" i2="X" l="FRE">
<s0>Baryum Lanthane Cobalt Oxyde Mixte</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>11</s5>
</fC03>
<fC03 i1="09" i2="X" l="ENG">
<s0>Barium Lanthanum Cobalt Oxides Mixed</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>11</s5>
</fC03>
<fC03 i1="09" i2="X" l="SPA">
<s0>Mixto</s0>
<s2>NC</s2>
<s2>NA</s2>
<s5>11</s5>
</fC03>
<fC03 i1="10" i2="X" l="FRE">
<s0>Approximation densité locale</s0>
<s5>12</s5>
</fC03>
<fC03 i1="10" i2="X" l="ENG">
<s0>Local density approximation</s0>
<s5>12</s5>
</fC03>
<fC03 i1="10" i2="X" l="SPA">
<s0>Aproximación densidad local</s0>
<s5>12</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Approximation gradient généralisé</s0>
<s5>13</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Generalized gradient approximation</s0>
<s5>13</s5>
</fC03>
<fN21>
<s1>195</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

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