Anomalous thermal redistribution of beryllium implanted in InGaAs: a possible interaction with extended defects
Identifieur interne : 00F901 ( Main/Repository ); précédent : 00F900; suivant : 00F902Anomalous thermal redistribution of beryllium implanted in InGaAs: a possible interaction with extended defects
Auteurs : RBID : Pascal:02-0559331Descripteurs français
- Pascal (Inist)
- Etude expérimentale, Semiconducteur III-V, Indium arséniure, Gallium arséniure, Couche mince, Couche épitaxique, Implantation ion, Phosphore ion, Dopage cristal, Addition béryllium, Recuit thermique rapide, Profil dopage, SIMS, Diffusion(transport), Hétérodiffusion, Interaction défaut cristallin, Simulation ordinateur, 6855L, InGaAs:Be P, As Ga In.
English descriptors
- KwdEn :
- Beryllium additions, Computerized simulation, Crystal defect interaction, Crystal doping, Diffusion, Doping profiles, Epitaxial layers, Experimental study, Gallium arsenides, III-V semiconductors, Impurity diffusion, Indium arsenides, Ion implantation, Phosphorus ions, Rapid thermal annealing, SIMS, Thin films.
Abstract
Phosphorus and beryllium have been coimplanted in InGaAs. Various anneals have been performed in the temperature range of 745-826°C. The secondary ion mass spectrometry measurements have revealed anomalous redistribution of the beryllium dopant: "up-hill" Be diffusion profiles have been observed. The observations of as-implanted profiles suggest that these anomalous beryllium peaks are due to beryllium trapping by the extended defects generated by the P implantation. A good agreement has been obtained between the experimental data and simulated profiles.
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Pascal:02-0559331Le document en format XML
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<author><name sortKey="Ketata, M" uniqKey="Ketata M">M. Ketata</name>
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<profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Beryllium additions</term>
<term>Computerized simulation</term>
<term>Crystal defect interaction</term>
<term>Crystal doping</term>
<term>Diffusion</term>
<term>Doping profiles</term>
<term>Epitaxial layers</term>
<term>Experimental study</term>
<term>Gallium arsenides</term>
<term>III-V semiconductors</term>
<term>Impurity diffusion</term>
<term>Indium arsenides</term>
<term>Ion implantation</term>
<term>Phosphorus ions</term>
<term>Rapid thermal annealing</term>
<term>SIMS</term>
<term>Thin films</term>
</keywords>
<keywords scheme="Pascal" xml:lang="fr"><term>Etude expérimentale</term>
<term>Semiconducteur III-V</term>
<term>Indium arséniure</term>
<term>Gallium arséniure</term>
<term>Couche mince</term>
<term>Couche épitaxique</term>
<term>Implantation ion</term>
<term>Phosphore ion</term>
<term>Dopage cristal</term>
<term>Addition béryllium</term>
<term>Recuit thermique rapide</term>
<term>Profil dopage</term>
<term>SIMS</term>
<term>Diffusion(transport)</term>
<term>Hétérodiffusion</term>
<term>Interaction défaut cristallin</term>
<term>Simulation ordinateur</term>
<term>6855L</term>
<term>InGaAs:Be P</term>
<term>As Ga In</term>
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<front><div type="abstract" xml:lang="en">Phosphorus and beryllium have been coimplanted in InGaAs. Various anneals have been performed in the temperature range of 745-826°C. The secondary ion mass spectrometry measurements have revealed anomalous redistribution of the beryllium dopant: "up-hill" Be diffusion profiles have been observed. The observations of as-implanted profiles suggest that these anomalous beryllium peaks are due to beryllium trapping by the extended defects generated by the P implantation. A good agreement has been obtained between the experimental data and simulated profiles.</div>
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<fC01 i1="01" l="ENG"><s0>Phosphorus and beryllium have been coimplanted in InGaAs. Various anneals have been performed in the temperature range of 745-826°C. The secondary ion mass spectrometry measurements have revealed anomalous redistribution of the beryllium dopant: "up-hill" Be diffusion profiles have been observed. The observations of as-implanted profiles suggest that these anomalous beryllium peaks are due to beryllium trapping by the extended defects generated by the P implantation. A good agreement has been obtained between the experimental data and simulated profiles.</s0>
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