Interdiffusion of III-V semiconductors heterostructures : effects of ion implantation and doping

Photoluminescence coupled with repetitive thermal annealing has been used to determine diffusion coefficients for intermixing in In0.2Ga0.8As/GaAs and GaAs/Al0.2Ga0.8As 100A single quantum wells and to study the effects of doping with silicon and beryllium and of ion implantation on the interdiffusi...

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Main Author: Bradley, I. V.
Published: University of Surrey 1993
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Online Access:http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.335632
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spelling ndltd-bl.uk-oai-ethos.bl.uk-3356322018-04-04T03:26:55ZInterdiffusion of III-V semiconductors heterostructures : effects of ion implantation and dopingBradley, I. V.1993Photoluminescence coupled with repetitive thermal annealing has been used to determine diffusion coefficients for intermixing in In0.2Ga0.8As/GaAs and GaAs/Al0.2Ga0.8As 100A single quantum wells and to study the effects of doping with silicon and beryllium and of ion implantation on the interdiffusion. It has been shown that the diffusion obeys Pick's law and that doping concentrations of beryllium up to 2.5 x 1019 cm-3 and silicon up to 10 18 cm-3 have no effect on the interdiffusion coefficients in either material system. For the In0.2Ga0.8As/GaAs system it was shown that following implantation and annealing there was a fast interdiffusion process which is independent of implant ion species and anneal temperature. This is thought to be due to recovery of the crystals from implant damage. After this rapid process, it was found that neither gallium nor krypton ions had any further effects on the interdiffusion. However, following arsenic implantation an additional enhanced region of interdiffusion coefficient was observed, with diffusion coefficients an order of magnitude greater than that of a control unimplanted sample. This enhancement is thought to be due to the creation of group in vacancies by the implanted arsenic atoms moving onto group V sites. This fast process was transient in nature returning to that of the unimplanted samples after the well has broadened by about 85A. An activation energy for the diffusion process of 3.7 +/- 0.1 eV was measured over a temperature range of 750-1050°C. This was found to be independent of implanted ion or dopant incorporated in the samples, indicating that the same process controls the interdiffusion in all cases. Similar results were found for the GaAs/Al0.2Ga0.8As system.530.41Solid-state physicsUniversity of Surreyhttp://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.335632http://epubs.surrey.ac.uk/842950/Electronic Thesis or Dissertation
collection NDLTD
sources NDLTD
topic 530.41
Solid-state physics
spellingShingle 530.41
Solid-state physics
Bradley, I. V.
Interdiffusion of III-V semiconductors heterostructures : effects of ion implantation and doping
description Photoluminescence coupled with repetitive thermal annealing has been used to determine diffusion coefficients for intermixing in In0.2Ga0.8As/GaAs and GaAs/Al0.2Ga0.8As 100A single quantum wells and to study the effects of doping with silicon and beryllium and of ion implantation on the interdiffusion. It has been shown that the diffusion obeys Pick's law and that doping concentrations of beryllium up to 2.5 x 1019 cm-3 and silicon up to 10 18 cm-3 have no effect on the interdiffusion coefficients in either material system. For the In0.2Ga0.8As/GaAs system it was shown that following implantation and annealing there was a fast interdiffusion process which is independent of implant ion species and anneal temperature. This is thought to be due to recovery of the crystals from implant damage. After this rapid process, it was found that neither gallium nor krypton ions had any further effects on the interdiffusion. However, following arsenic implantation an additional enhanced region of interdiffusion coefficient was observed, with diffusion coefficients an order of magnitude greater than that of a control unimplanted sample. This enhancement is thought to be due to the creation of group in vacancies by the implanted arsenic atoms moving onto group V sites. This fast process was transient in nature returning to that of the unimplanted samples after the well has broadened by about 85A. An activation energy for the diffusion process of 3.7 +/- 0.1 eV was measured over a temperature range of 750-1050°C. This was found to be independent of implanted ion or dopant incorporated in the samples, indicating that the same process controls the interdiffusion in all cases. Similar results were found for the GaAs/Al0.2Ga0.8As system.
author Bradley, I. V.
author_facet Bradley, I. V.
author_sort Bradley, I. V.
title Interdiffusion of III-V semiconductors heterostructures : effects of ion implantation and doping
title_short Interdiffusion of III-V semiconductors heterostructures : effects of ion implantation and doping
title_full Interdiffusion of III-V semiconductors heterostructures : effects of ion implantation and doping
title_fullStr Interdiffusion of III-V semiconductors heterostructures : effects of ion implantation and doping
title_full_unstemmed Interdiffusion of III-V semiconductors heterostructures : effects of ion implantation and doping
title_sort interdiffusion of iii-v semiconductors heterostructures : effects of ion implantation and doping
publisher University of Surrey
publishDate 1993
url http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.335632
work_keys_str_mv AT bradleyiv interdiffusionofiiivsemiconductorsheterostructureseffectsofionimplantationanddoping
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