Serveur d'exploration sur l'Indium

Attention, ce site est en cours de développement !
Attention, site généré par des moyens informatiques à partir de corpus bruts.
Les informations ne sont donc pas validées.

First-principles study of the structural properties and magnetism of R2CoIn8 (R=Y, Pr, Nd, and Dy) intermetallic compounds

Identifieur interne : 001B74 ( Main/Repository ); précédent : 001B73; suivant : 001B75

First-principles study of the structural properties and magnetism of R2CoIn8 (R=Y, Pr, Nd, and Dy) intermetallic compounds

Auteurs : RBID : Pascal:12-0213104

Descripteurs français

English descriptors

Abstract

The electronic structure of R2CoIn8 (R=Y, Pr, Nd, and Dy) intermetallic compounds is calculated from first principles based on the density functional theory (DFT). The Kohn-Sham single-particle equations of the DFT are solved using two independent computational methods, namely APW+lo and FPLO. First the structural properties of Y2CoIn8 are studied. Good agreement of calculated equilibrium volume and c/a ratio with the experimental data is found. Also we minimize the forces at equilibrium volume and calculate the symmetry-free structural parameters of the space group P4/mmm for Y2CoIn8. In Y2CoIn8, the Co 3d states are almost fully occupied and situated below the Fermi level. We applied the fixed-spin-moment method and a stable paramagnetic ground state for Y3CoIn8 was found. Finally, the crystal field (CF) parameters were calculated for R=Pr, Nd and Dy from first principles. The microscopic tetragonal CF Hamiltonian was diagonalized and the obtained eigenvalues and eigenfunctions were used to predict the anisotropy of the magnetic properties of R2CoIn8 single crystals.

Links toward previous steps (curation, corpus...)


Links to Exploration step

Pascal:12-0213104

Le document en format XML

<record>
<TEI>
<teiHeader>
<fileDesc>
<titleStmt>
<title xml:lang="en" level="a">First-principles study of the structural properties and magnetism of R
<sub>2</sub>
CoIn
<sub>8</sub>
(R=Y, Pr, Nd, and Dy) intermetallic compounds</title>
<author>
<name sortKey="Divis, M" uniqKey="Divis M">M. Divis</name>
<affiliation wicri:level="1">
<inist:fA14 i1="01">
<s1>Faculty of Mathematics and Physics, Charles University, Department of Condensed Matter Physics, Ke Karlovu 5</s1>
<s2>121 16 Prague</s2>
<s3>CZE</s3>
<sZ>1 aut.</sZ>
</inist:fA14>
<country>République tchèque</country>
<wicri:noRegion>121 16 Prague</wicri:noRegion>
</affiliation>
</author>
</titleStmt>
<publicationStmt>
<idno type="inist">12-0213104</idno>
<date when="2012">2012</date>
<idno type="stanalyst">PASCAL 12-0213104 INIST</idno>
<idno type="RBID">Pascal:12-0213104</idno>
<idno type="wicri:Area/Main/Corpus">001D82</idno>
<idno type="wicri:Area/Main/Repository">001B74</idno>
</publicationStmt>
<seriesStmt>
<idno type="ISSN">0921-4526</idno>
<title level="j" type="abbreviated">Physica, B Condens. matter</title>
<title level="j" type="main">Physica. B, Condensed matter</title>
</seriesStmt>
</fileDesc>
<profileDesc>
<textClass>
<keywords scheme="KwdEn" xml:lang="en">
<term>Band structure</term>
<term>Cobalt alloys</term>
<term>Crystal field</term>
<term>Density functional method</term>
<term>Electronic density of states</term>
<term>Hamiltonians</term>
<term>Indium alloys</term>
<term>Intermetallic compounds</term>
<term>Magnetic anisotropy</term>
<term>Magnetic susceptibility</term>
<term>Magnetization</term>
<term>Monocrystals</term>
<term>Rare earth alloys</term>
<term>Ternary alloys</term>
<term>Transition element alloys</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr">
<term>Méthode fonctionnelle densité</term>
<term>Densité état électron</term>
<term>Anisotropie magnétique</term>
<term>Aimantation</term>
<term>Susceptibilité magnétique</term>
<term>Champ cristallin</term>
<term>Hamiltonien</term>
<term>Lanthanide alliage</term>
<term>Structure bande</term>
<term>Cobalt alliage</term>
<term>Composé intermétallique</term>
<term>Indium alliage</term>
<term>Alliage ternaire</term>
<term>Monocristal</term>
<term>Métal transition alliage</term>
</keywords>
</textClass>
</profileDesc>
</teiHeader>
<front>
<div type="abstract" xml:lang="en">The electronic structure of R
<sub>2</sub>
CoIn
<sub>8</sub>
(R=Y, Pr, Nd, and Dy) intermetallic compounds is calculated from first principles based on the density functional theory (DFT). The Kohn-Sham single-particle equations of the DFT are solved using two independent computational methods, namely APW+lo and FPLO. First the structural properties of Y
<sub>2</sub>
CoIn
<sub>8</sub>
are studied. Good agreement of calculated equilibrium volume and c/a ratio with the experimental data is found. Also we minimize the forces at equilibrium volume and calculate the symmetry-free structural parameters of the space group P4/mmm for Y
<sub>2</sub>
CoIn
<sub>8</sub>
. In Y
<sub>2</sub>
CoIn
<sub>8</sub>
, the Co 3d states are almost fully occupied and situated below the Fermi level. We applied the fixed-spin-moment method and a stable paramagnetic ground state for Y
<sub>3</sub>
CoIn
<sub>8</sub>
was found. Finally, the crystal field (CF) parameters were calculated for R
<sub>=</sub>
Pr, Nd and Dy from first principles. The microscopic tetragonal CF Hamiltonian was diagonalized and the obtained eigenvalues and eigenfunctions were used to predict the anisotropy of the magnetic properties of R
<sub>2</sub>
CoIn
<sub>8</sub>
single crystals.</div>
</front>
</TEI>
<inist>
<standard h6="B">
<pA>
<fA01 i1="01" i2="1">
<s0>0921-4526</s0>
</fA01>
<fA03 i2="1">
<s0>Physica, B Condens. matter</s0>
</fA03>
<fA05>
<s2>407</s2>
</fA05>
<fA06>
<s2>13</s2>
</fA06>
<fA08 i1="01" i2="1" l="ENG">
<s1>First-principles study of the structural properties and magnetism of R
<sub>2</sub>
CoIn
<sub>8</sub>
(R=Y, Pr, Nd, and Dy) intermetallic compounds</s1>
</fA08>
<fA11 i1="01" i2="1">
<s1>DIVIS (M.)</s1>
</fA11>
<fA14 i1="01">
<s1>Faculty of Mathematics and Physics, Charles University, Department of Condensed Matter Physics, Ke Karlovu 5</s1>
<s2>121 16 Prague</s2>
<s3>CZE</s3>
<sZ>1 aut.</sZ>
</fA14>
<fA20>
<s1>2524-2526</s1>
</fA20>
<fA21>
<s1>2012</s1>
</fA21>
<fA23 i1="01">
<s0>ENG</s0>
</fA23>
<fA43 i1="01">
<s1>INIST</s1>
<s2>145B</s2>
<s5>354000509295700310</s5>
</fA43>
<fA44>
<s0>0000</s0>
<s1>© 2012 INIST-CNRS. All rights reserved.</s1>
</fA44>
<fA45>
<s0>9 ref.</s0>
</fA45>
<fA47 i1="01" i2="1">
<s0>12-0213104</s0>
</fA47>
<fA60>
<s1>P</s1>
</fA60>
<fA61>
<s0>A</s0>
</fA61>
<fA64 i1="01" i2="1">
<s0>Physica. B, Condensed matter</s0>
</fA64>
<fA66 i1="01">
<s0>GBR</s0>
</fA66>
<fC01 i1="01" l="ENG">
<s0>The electronic structure of R
<sub>2</sub>
CoIn
<sub>8</sub>
(R=Y, Pr, Nd, and Dy) intermetallic compounds is calculated from first principles based on the density functional theory (DFT). The Kohn-Sham single-particle equations of the DFT are solved using two independent computational methods, namely APW+lo and FPLO. First the structural properties of Y
<sub>2</sub>
CoIn
<sub>8</sub>
are studied. Good agreement of calculated equilibrium volume and c/a ratio with the experimental data is found. Also we minimize the forces at equilibrium volume and calculate the symmetry-free structural parameters of the space group P4/mmm for Y
<sub>2</sub>
CoIn
<sub>8</sub>
. In Y
<sub>2</sub>
CoIn
<sub>8</sub>
, the Co 3d states are almost fully occupied and situated below the Fermi level. We applied the fixed-spin-moment method and a stable paramagnetic ground state for Y
<sub>3</sub>
CoIn
<sub>8</sub>
was found. Finally, the crystal field (CF) parameters were calculated for R
<sub>=</sub>
Pr, Nd and Dy from first principles. The microscopic tetragonal CF Hamiltonian was diagonalized and the obtained eigenvalues and eigenfunctions were used to predict the anisotropy of the magnetic properties of R
<sub>2</sub>
CoIn
<sub>8</sub>
single crystals.</s0>
</fC01>
<fC02 i1="01" i2="3">
<s0>001B70E30C</s0>
</fC02>
<fC02 i1="02" i2="3">
<s0>001B70E60E</s0>
</fC02>
<fC02 i1="03" i2="3">
<s0>001B70A70C</s0>
</fC02>
<fC02 i1="04" i2="3">
<s0>001B70A20L</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="3" l="FRE">
<s0>Densité état électron</s0>
<s5>03</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG">
<s0>Electronic density of states</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE">
<s0>Anisotropie magnétique</s0>
<s5>04</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG">
<s0>Magnetic anisotropy</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE">
<s0>Aimantation</s0>
<s5>05</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG">
<s0>Magnetization</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE">
<s0>Susceptibilité magnétique</s0>
<s5>06</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG">
<s0>Magnetic susceptibility</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="3" l="FRE">
<s0>Champ cristallin</s0>
<s5>08</s5>
</fC03>
<fC03 i1="06" i2="3" l="ENG">
<s0>Crystal field</s0>
<s5>08</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE">
<s0>Hamiltonien</s0>
<s5>10</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG">
<s0>Hamiltonians</s0>
<s5>10</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE">
<s0>Lanthanide alliage</s0>
<s5>13</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG">
<s0>Rare earth alloys</s0>
<s5>13</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE">
<s0>Structure bande</s0>
<s5>14</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG">
<s0>Band structure</s0>
<s5>14</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE">
<s0>Cobalt alliage</s0>
<s5>15</s5>
</fC03>
<fC03 i1="10" i2="3" l="ENG">
<s0>Cobalt alloys</s0>
<s5>15</s5>
</fC03>
<fC03 i1="11" i2="3" l="FRE">
<s0>Composé intermétallique</s0>
<s5>16</s5>
</fC03>
<fC03 i1="11" i2="3" l="ENG">
<s0>Intermetallic compounds</s0>
<s5>16</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE">
<s0>Indium alliage</s0>
<s5>17</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG">
<s0>Indium alloys</s0>
<s5>17</s5>
</fC03>
<fC03 i1="13" i2="3" l="FRE">
<s0>Alliage ternaire</s0>
<s5>18</s5>
</fC03>
<fC03 i1="13" i2="3" l="ENG">
<s0>Ternary alloys</s0>
<s5>18</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE">
<s0>Monocristal</s0>
<s5>19</s5>
</fC03>
<fC03 i1="14" i2="3" l="ENG">
<s0>Monocrystals</s0>
<s5>19</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE">
<s0>Métal transition alliage</s0>
<s5>48</s5>
</fC03>
<fC03 i1="15" i2="3" l="ENG">
<s0>Transition element alloys</s0>
<s5>48</s5>
</fC03>
<fN21>
<s1>163</s1>
</fN21>
</pA>
</standard>
</inist>
</record>

Pour manipuler ce document sous Unix (Dilib)

EXPLOR_STEP=IndiumV3/Data/Main/Repository
HfdSelect -h $EXPLOR_STEP/biblio.hfd -nk 001B74 | SxmlIndent | more

Ou

HfdSelect -h $EXPLOR_AREA/Data/Main/Repository/biblio.hfd -nk 001B74 | SxmlIndent | more

Pour mettre un lien sur cette page dans le réseau Wicri

{{Explor lien
   |wiki=   *** parameter Area/wikiCode missing *** 
   |area=    IndiumV3
   |flux=    Main
   |étape=   Repository
   |type=    RBID
   |clé=     Pascal:12-0213104
   |texte=   First-principles study of the structural properties and magnetism of R2CoIn8 (R=Y, Pr, Nd, and Dy) intermetallic compounds
}}

Wicri

This area was generated with Dilib version V0.5.77.
Data generation: Mon Jun 9 10:27:54 2014. Site generation: Thu Mar 7 16:19:59 2024