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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 77 (1995), S. 5418-5421 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The dependence of S impurity incorporation into GaAs vs growth rate, and substrate temperature has been investigated during vapor phase epitaxial growth. The specific technique used, close space vapor transport, has been selected to allow the growth rate Vg and the substrate temperature θ to vary independently and in very large ranges. The concentration ND of incorporated impurities has been determined for a variety of values of Vg and θ, using an electrical method. Comparison of the experimental data with a simple model gives the variation of the sticking coefficient versus temperature. The model assumes that the impurities incorporated are those which stick on the surface during the time a monolayer is grown, when desorption can be neglected during this time. This sticking coefficient is thermally activated with an activation energy of 2 eV. The agreement between the experimental data and the variation of ND vs Vg and θ deduced from this model, confirms its validity and demonstrates that high purity GaAs can be grown by this technique under high growth rate conditions. © 1995 American Institute of Physics.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 68 (1990), S. 6274-6278 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Semi-insulating GaAs material results from the compensation of residual acceptor impurities and intrinsic defects by the so-called EL2 donor defects which possess a level at midgap. A semi-insulating layer can therefore be produced if it is possible to introduce a large enough concentration of EL2 defects. We describe a vapor-phase epitaxy technique which allows to introduce an EL2 concentration in the range 1015–1016 cm−3. This technique is made to reach very large growth rates, based on the fact that the EL2 concentration increases with the growth rate. The variation of the EL2 concentration versus the various growth parameters (substrate temperature, partial pressure, growth rate) have been monitored. The mechanism by which the incorporation of EL2 defects occurs has been determined, thus allowing one to get a given EL2 concentration reproducibly. This technique of growth, being inexpensive and fast, requiring no toxic gases, appears to be a reasonable alternative to the production of semi-insulating substrates.
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 69 (1991), S. 284-290 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The evolution of the deep level transient spectroscopy spectrum associated with the EL2 defect in epitaxial as well as bulk GaAs materials when they are contaminated by oxygen has been examined in detail. The degree of contamination is evaluated by ion mass spectroscopy. It has been observed that, as previously noticed, the EL2 spectrum contains two components. From the variations of the amplitude of these components versus time at different temperatures and versus electric field, it is concluded that, while one of these components is associated with the EL2 defect, the other one originates from the interaction of EL2 with interstitial oxygen. The deformation of the EL2 spectrum which is currently observed when using aluminum Schottky barriers is then understood as an effect of oxygen contamination and not due, as previously argued, to changes in the barrier characteristics.
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 91 (2002), S. 5923-5928 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The reactivation kinetics of the acceptor behavior of carbon, its dependence on dopant precursors, doping level, layer thickness, and annealing temperature, as well as the behavior of carbon-hydrogen complexes in GaAs grown by metalorganic chemical vapor deposition are studied. Independent of the carbon source, in the "as grown" material, systematically carbon hydrogen complexes are present and the hole concentration is lower than the corresponding carbon concentration. The carbon reactivation kinetics was achieved by ex situ rapid thermal annealing through a series of multistage annealing experiments and assessed at each annealing stage by infrared absorption, hydrogen secondary ion mass spectroscopy profiling, and hole concentration measurements. Carbon reactivation occurs solely by the debonding of hydrogen from the isolated carbon acceptor and its out-diffusion from the sample. The carbon reactivation kinetics can be treated as a first order one with an activation energy, Ea=1.42±0.01 eV, independent of doping precursors, doping level, and layer thickness. The reactivation constant results to decrease as doping level and layer thickness increase. An empirical formula has been obtained that allows one to calculate the reactivation constant as a function of the carbon doping, layer thickness, and annealing temperature, allowing one to determine the optimal carbon reactivation conditions for any C:GaAs layer. © 2002 American Institute of Physics.
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  • 5
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 58 (1985), S. 3652-3654 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Close spaced vapor transport (CSVT) epitaxial layers have been grown under water vapor partial pressure p ranging from 5×10−2 to 5 mm Hg for source temperatures of 800 and 850 °C and a substrate temperature of 730 °C, using undoped high-purity GaAs as source material and 〈100〉 chromium doped high-resistivity GaAs as substrate. From Hall measurements, all layers were found to be n-type with a majority carrier concentration in the range of (2–3) ×1017 cm−3 and a mobility 3100–3600 cm2 V−1 s−1 as p varies from 5.0 to 5×10−2 mm Hg. Photoluminescence measurements show the following dominant recombination processes: an exitonic peak at 1.514 eV, a free band acceptor at 1.498 eV, a donor acceptor at 1.490 eV, and two peaks involving complexes at 1.47 and 1.42 eV. These peaks depend on the water vapor pressure: for low values of p only the exitonic peaks exist; as p increases the photoluminescence becomes less efficient until it disappears for p=5.0 mm Hg. This study shows that CSVT-GaAs epilayers grown under proper conditions have high quality and could be used for producing some electronic devices.
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  • 6
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 77 (2000), S. 1164-1166 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The reactivation kinetics of the acceptor behavior of carbon in GaAs layers has been studied. The reactivation was achieved by ex situ rapid thermal annealing. To follow the carbon reactivation process, a multistage annealing experiment was performed, with changes in the sample carrier concentration monitored at each stage. An analysis of these data indicates that carbon reactivation follows a first-order kinetics process that can be explained by a model which includes the effects of dopant repassivation by hydrogen retrapping during hydrogen out-diffusion, and a dependence of the attempt frequency with the carbon concentration. The reactivation occurs with an activation energy of 1.41 eV. © 2000 American Institute of Physics.
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  • 7
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 79 (2001), S. 3095-3097 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Carbon doping efficiency in GaAs grown by metalorganic chemical vapor deposition using intrinsic and extrinsic doping sources is studied. Independent of the carbon source, carbon hydrogen complexes are systematically present and depending on the growth conditions, carbon dimers can be present and form complexes with hydrogen as well. Carbon–hydrogen related complexes and dimers reduce the hole concentration decreasing the doping efficiency. Additionally, the carbon dimer introduces a deep level, decreases the hole mobility and hydrogen bonds stronger to it than to isolated carbon. Depending on the growth conditions it is possible to reach 100% doping efficiency with high hole mobility. © 2001 American Institute of Physics.
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  • 8
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 51 (1987), S. 2004-2006 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: For the first time gallium arsenide field-effect transistors have been made using epitaxial layers grown by the close spaced vapor transport technique (CSVT). The layers were unintentionally doped and their free-carrier concentration was adjusted through the growth parameters to around 1017 cm−3. For the growth of the layers, water vapor was used as transporting gas. This transistor confirms the capability of the simplest and most inexpensive epitaxial technique (CSVT) for growing device quality gallium arsenide epitaxial layers.
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  • 9
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 84 (1998), S. 1572-1578 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: InP epitaxial layers have been grown at high growth rates by vapor phase reactive transport. A systematic study of the influence of growth conditions on the growth rate, surface morphology, and photoluminescence properties of the grown materials has been performed. The results show that the growth rate can be controlled at least between 0.3 and 75 μm per hour, the latter being over 75 times of the growth rate obtained with the usual techniques. The changes of the surface morphology of the layers with the growth conditions have been understood and layers having mirror-like surfaces can be grown for any growth rate. The mass transport mechanism occurs through three chemical reactions whose activation energies have been determined and a reliable model for the growth rate as a function of the growth conditions is now available. Double diffraction x-ray measurements demonstrate that the layers are characterized by a peak whose width at half maximum is 18 arcsec, even for the highest growth rates. Low temperature luminescence exhibits transitions involving free and bound excitons, and shallow donors and acceptors. C and Zn are identified as the only residual acceptors and no radiative deep levels are detected. Depending on the growth conditions, C or Zn are incorporated preferentially as the dominant acceptor. The intensity ratio of the excitonic transition to the transition involving Zn as acceptor varies exponentially with the growth temperature. © 1998 American Institute of Physics.
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  • 10
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Journal of Crystal Growth 68 (1984), S. 671-676 
    ISSN: 0022-0248
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Chemistry and Pharmacology , Geosciences , Physics
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