Positron annihilation in narrow-gap semiconductors
Identifieur interne : 01C352 ( Main/Repository ); précédent : 01C351; suivant : 01C353Positron annihilation in narrow-gap semiconductors
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Abstract
The valence electron and positron charge densities in InAs and InSb are obtained from wave functions derived in a model pseudopotential band-structure calculation. It is found that the positron density is maximum in the open interstices and is excluded not only, as usual, from the ion cores but also to a considerable degree from the valence bonds. Electron-positron momentum densities are calculated for the (001-110) plane. The results are used to analyze the positron effect in narrow-gap semiconductors
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<author><name sortKey="Bouarissa, N" uniqKey="Bouarissa N">N. Bouarissa</name>
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<author><name sortKey="West, R N" uniqKey="West R">R. N. West</name>
<affiliation wicri:level="1"><inist:fA14 i1="02"><s1>Univ. Texas Arlington, dep. physics</s1>
<s2>Arlington TX 80900</s2>
<s3>USA</s3>
<sZ>2 aut.</sZ>
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<country>États-Unis</country>
<wicri:noRegion>Arlington TX 80900</wicri:noRegion>
</affiliation>
</author>
<author><name sortKey="Aourag, H" uniqKey="Aourag H">H. Aourag</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Univ. Sidi-Bel-Abbes, dep. physics, computational materials sci. lab.</s1>
<s2>Sidi-Bel-Abbes 22000</s2>
<s3>ALB</s3>
<sZ>1 aut.</sZ>
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<title level="j" type="main">Physica status solidi. B. Basic research</title>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Annihilation</term>
<term>Binary compounds</term>
<term>Charge density</term>
<term>Electronic structure</term>
<term>Energy-level density</term>
<term>III-V semiconductors</term>
<term>Indium antimonides</term>
<term>Indium arsenides</term>
<term>Momentum density</term>
<term>Positron probes</term>
<term>Pseudopotential</term>
<term>Theoretical study</term>
<term>Valence electron</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Etude théorique</term>
<term>Structure électronique</term>
<term>Annihilation</term>
<term>Sonde positonique</term>
<term>Densité niveau énergie</term>
<term>Electron valence</term>
<term>Densité quantité mouvement</term>
<term>Pseudopotentiel</term>
<term>Densité charge</term>
<term>Semiconducteur III-V</term>
<term>Indium arséniure</term>
<term>Indium antimoniure</term>
<term>Composé binaire</term>
<term>7120F</term>
<term>7870B</term>
<term>InAs</term>
<term>InSb</term>
<term>As In</term>
<term>In Sb</term>
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<front><div type="abstract" xml:lang="en">The valence electron and positron charge densities in InAs and InSb are obtained from wave functions derived in a model pseudopotential band-structure calculation. It is found that the positron density is maximum in the open interstices and is excluded not only, as usual, from the ion cores but also to a considerable degree from the valence bonds. Electron-positron momentum densities are calculated for the (001-110) plane. The results are used to analyze the positron effect in narrow-gap semiconductors</div>
</front>
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<fA05><s2>188</s2>
</fA05>
<fA06><s2>2</s2>
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<fA08 i1="01" i2="1" l="ENG"><s1>Positron annihilation in narrow-gap semiconductors</s1>
</fA08>
<fA11 i1="01" i2="1"><s1>BOUARISSA (N.)</s1>
</fA11>
<fA11 i1="02" i2="1"><s1>WEST (R. N.)</s1>
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<fA11 i1="03" i2="1"><s1>AOURAG (H.)</s1>
</fA11>
<fA14 i1="01"><s1>Univ. Sidi-Bel-Abbes, dep. physics, computational materials sci. lab.</s1>
<s2>Sidi-Bel-Abbes 22000</s2>
<s3>ALB</s3>
<sZ>1 aut.</sZ>
<sZ>3 aut.</sZ>
</fA14>
<fA14 i1="02"><s1>Univ. Texas Arlington, dep. physics</s1>
<s2>Arlington TX 80900</s2>
<s3>USA</s3>
<sZ>2 aut.</sZ>
</fA14>
<fA20><s1>723-734</s1>
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<fA21><s1>1995</s1>
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</fA66>
<fC01 i1="01" l="ENG"><s0>The valence electron and positron charge densities in InAs and InSb are obtained from wave functions derived in a model pseudopotential band-structure calculation. It is found that the positron density is maximum in the open interstices and is excluded not only, as usual, from the ion cores but also to a considerable degree from the valence bonds. Electron-positron momentum densities are calculated for the (001-110) plane. The results are used to analyze the positron effect in narrow-gap semiconductors</s0>
</fC01>
<fC02 i1="01" i2="3"><s0>001B70A20F</s0>
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<fC02 i1="02" i2="3"><s0>001B70H70B</s0>
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<s5>01</s5>
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<s5>01</s5>
</fC03>
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<s5>02</s5>
</fC03>
<fC03 i1="02" i2="3" l="ENG"><s0>Electronic structure</s0>
<s5>02</s5>
</fC03>
<fC03 i1="03" i2="3" l="FRE"><s0>Annihilation</s0>
<s5>03</s5>
</fC03>
<fC03 i1="03" i2="3" l="ENG"><s0>Annihilation</s0>
<s5>03</s5>
</fC03>
<fC03 i1="04" i2="3" l="FRE"><s0>Sonde positonique</s0>
<s5>04</s5>
</fC03>
<fC03 i1="04" i2="3" l="ENG"><s0>Positron probes</s0>
<s5>04</s5>
</fC03>
<fC03 i1="05" i2="3" l="FRE"><s0>Densité niveau énergie</s0>
<s5>05</s5>
</fC03>
<fC03 i1="05" i2="3" l="ENG"><s0>Energy-level density</s0>
<s5>05</s5>
</fC03>
<fC03 i1="06" i2="X" l="FRE"><s0>Electron valence</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="X" l="ENG"><s0>Valence electron</s0>
<s5>06</s5>
</fC03>
<fC03 i1="06" i2="X" l="SPA"><s0>Electrón valencia</s0>
<s5>06</s5>
</fC03>
<fC03 i1="07" i2="3" l="FRE"><s0>Densité quantité mouvement</s0>
<s5>07</s5>
</fC03>
<fC03 i1="07" i2="3" l="ENG"><s0>Momentum density</s0>
<s5>07</s5>
</fC03>
<fC03 i1="08" i2="3" l="FRE"><s0>Pseudopotentiel</s0>
<s5>08</s5>
</fC03>
<fC03 i1="08" i2="3" l="ENG"><s0>Pseudopotential</s0>
<s5>08</s5>
</fC03>
<fC03 i1="09" i2="3" l="FRE"><s0>Densité charge</s0>
<s5>09</s5>
</fC03>
<fC03 i1="09" i2="3" l="ENG"><s0>Charge density</s0>
<s5>09</s5>
</fC03>
<fC03 i1="10" i2="3" l="FRE"><s0>Semiconducteur III-V</s0>
<s5>13</s5>
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<s5>13</s5>
</fC03>
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<s2>NK</s2>
<s5>14</s5>
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<s2>NK</s2>
<s5>14</s5>
</fC03>
<fC03 i1="12" i2="3" l="FRE"><s0>Indium antimoniure</s0>
<s2>NK</s2>
<s5>15</s5>
</fC03>
<fC03 i1="12" i2="3" l="ENG"><s0>Indium antimonides</s0>
<s2>NK</s2>
<s5>15</s5>
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<s5>16</s5>
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<fC03 i1="13" i2="3" l="ENG"><s0>Binary compounds</s0>
<s5>16</s5>
</fC03>
<fC03 i1="14" i2="3" l="FRE"><s0>7120F</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC03 i1="15" i2="3" l="FRE"><s0>7870B</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>57</s5>
</fC03>
<fC03 i1="16" i2="3" l="FRE"><s0>InAs</s0>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fC03 i1="17" i2="3" l="FRE"><s0>InSb</s0>
<s4>INC</s4>
<s5>93</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>As In</s0>
<s4>INC</s4>
<s5>94</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>In Sb</s0>
<s4>INC</s4>
<s5>95</s5>
</fC03>
<fC07 i1="01" i2="3" l="FRE"><s0>Composé minéral</s0>
<s5>17</s5>
</fC07>
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<s5>17</s5>
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<fN21><s1>156</s1>
</fN21>
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