Determination of beryllium and self-interstitial diffusion parameters in InGaAs
Identifieur interne : 00D784 ( Main/Repository ); précédent : 00D783; suivant : 00D785Determination of beryllium and self-interstitial diffusion parameters in InGaAs
Auteurs : RBID : Pascal:03-0271097Descripteurs français
- Pascal (Inist)
- Etude expérimentale, Croissance cristalline en phase vapeur, Méthode GSMBE, Couche épitaxique, Indium arséniure, Gallium arséniure, Semiconducteur III-V, Dopage, Addition béryllium, Diffusion(transport), Diffusion impureté, Interstitiel, SIMS, Recuit thermique, Dépendance température, Modélisation, 8115H, 6855L, InGaAs:Be, As Ga In.
- Wicri :
- concept : Dopage.
English descriptors
- KwdEn :
Abstract
The diffusion of Be in InGaAs grown by gas source molecular beam epitaxy has been studied. The observed secondary ion mass spectrometry Be profiles, obtained for annealing cycles with a temperature range of 700-900°C, could be explained considering several forms of kick-out mechanism. The beryllium diffusion models in InGaAs have been obtained without a priori hypothesis on interstitial beryllium and self-interstitial. Moreover, the fitting procedure of experimental data has been described precisely. We conclude that two kick-out mechanisms lead to similar fittings of experimental profiles and may not be distinguishable using our experimental conditions.
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<record><TEI><teiHeader><fileDesc><titleStmt><title xml:lang="en" level="a">Determination of beryllium and self-interstitial diffusion parameters in InGaAs</title>
<author><name sortKey="Marcon, J" uniqKey="Marcon J">J. Marcon</name>
<affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Laboratoire Electronique Microtechnologie Instrumentation, LEMI-IUT-Université de Rouen, IUT de Rouen, UPRES 2654</s1>
<s2>76821 Mont Saint Aignan</s2>
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<sZ>2 aut.</sZ>
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<country>France</country>
<placeName><region type="region" nuts="2">Haute-Normandie</region>
<settlement type="city">Mont Saint Aignan</settlement>
</placeName>
<orgName type="university">Université de Rouen</orgName>
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<author><name sortKey="Ihaddadene, M" uniqKey="Ihaddadene M">M. Ihaddadene</name>
<affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Laboratoire Electronique Microtechnologie Instrumentation, LEMI-IUT-Université de Rouen, IUT de Rouen, UPRES 2654</s1>
<s2>76821 Mont Saint Aignan</s2>
<s3>FRA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
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<country>France</country>
<placeName><region type="region" nuts="2">Haute-Normandie</region>
<settlement type="city">Mont Saint Aignan</settlement>
</placeName>
<orgName type="university">Université de Rouen</orgName>
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</author>
<author><name sortKey="Ketata, K" uniqKey="Ketata K">K. Ketata</name>
<affiliation wicri:level="4"><inist:fA14 i1="01"><s1>Laboratoire Electronique Microtechnologie Instrumentation, LEMI-IUT-Université de Rouen, IUT de Rouen, UPRES 2654</s1>
<s2>76821 Mont Saint Aignan</s2>
<s3>FRA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
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<country>France</country>
<placeName><region type="region" nuts="2">Haute-Normandie</region>
<settlement type="city">Mont Saint Aignan</settlement>
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<title level="j" type="abbreviated">J. cryst. growth</title>
<title level="j" type="main">Journal of crystal growth</title>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Beryllium additions</term>
<term>Crystal growth from vapors</term>
<term>Diffusion</term>
<term>Doping</term>
<term>Epitaxial layers</term>
<term>Experimental study</term>
<term>GSMBE method</term>
<term>Gallium arsenides</term>
<term>III-V semiconductors</term>
<term>Impurity scattering</term>
<term>Indium arsenides</term>
<term>Interstitials</term>
<term>Modelling</term>
<term>SIMS</term>
<term>Temperature dependence</term>
<term>Thermal annealing</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Etude expérimentale</term>
<term>Croissance cristalline en phase vapeur</term>
<term>Méthode GSMBE</term>
<term>Couche épitaxique</term>
<term>Indium arséniure</term>
<term>Gallium arséniure</term>
<term>Semiconducteur III-V</term>
<term>Dopage</term>
<term>Addition béryllium</term>
<term>Diffusion(transport)</term>
<term>Diffusion impureté</term>
<term>Interstitiel</term>
<term>SIMS</term>
<term>Recuit thermique</term>
<term>Dépendance température</term>
<term>Modélisation</term>
<term>8115H</term>
<term>6855L</term>
<term>InGaAs:Be</term>
<term>As Ga In</term>
</keywords>
<keywords scheme="Wicri" type="concept" xml:lang="fr"><term>Dopage</term>
</keywords>
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<front><div type="abstract" xml:lang="en">The diffusion of Be in InGaAs grown by gas source molecular beam epitaxy has been studied. The observed secondary ion mass spectrometry Be profiles, obtained for annealing cycles with a temperature range of 700-900°C, could be explained considering several forms of kick-out mechanism. The beryllium diffusion models in InGaAs have been obtained without a priori hypothesis on interstitial beryllium and self-interstitial. Moreover, the fitting procedure of experimental data has been described precisely. We conclude that two kick-out mechanisms lead to similar fittings of experimental profiles and may not be distinguishable using our experimental conditions.</div>
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<fA08 i1="01" i2="1" l="ENG"><s1>Determination of beryllium and self-interstitial diffusion parameters in InGaAs</s1>
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<fA11 i1="02" i2="1"><s1>IHADDADENE (M.)</s1>
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<fA11 i1="03" i2="1"><s1>KETATA (K.)</s1>
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<fA14 i1="01"><s1>Laboratoire Electronique Microtechnologie Instrumentation, LEMI-IUT-Université de Rouen, IUT de Rouen, UPRES 2654</s1>
<s2>76821 Mont Saint Aignan</s2>
<s3>FRA</s3>
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<sZ>2 aut.</sZ>
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<fC01 i1="01" l="ENG"><s0>The diffusion of Be in InGaAs grown by gas source molecular beam epitaxy has been studied. The observed secondary ion mass spectrometry Be profiles, obtained for annealing cycles with a temperature range of 700-900°C, could be explained considering several forms of kick-out mechanism. The beryllium diffusion models in InGaAs have been obtained without a priori hypothesis on interstitial beryllium and self-interstitial. Moreover, the fitting procedure of experimental data has been described precisely. We conclude that two kick-out mechanisms lead to similar fittings of experimental profiles and may not be distinguishable using our experimental conditions.</s0>
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<s5>12</s5>
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<s5>12</s5>
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<s5>13</s5>
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<s5>13</s5>
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<s5>14</s5>
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<s5>18</s5>
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<s5>18</s5>
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<fC03 i1="17" i2="3" l="FRE"><s0>8115H</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>56</s5>
</fC03>
<fC03 i1="18" i2="3" l="FRE"><s0>6855L</s0>
<s2>PAC</s2>
<s4>INC</s4>
<s5>57</s5>
</fC03>
<fC03 i1="19" i2="3" l="FRE"><s0>InGaAs:Be</s0>
<s4>INC</s4>
<s5>92</s5>
</fC03>
<fC03 i1="20" i2="3" l="FRE"><s0>As Ga In</s0>
<s4>INC</s4>
<s5>93</s5>
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