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Characteristics of carbon doped InGaAs using carbontetrabromide by metalorganic molecular beam epitaxy

Identifieur interne : 002038 ( Istex/Curation ); précédent : 002037; suivant : 002039

Characteristics of carbon doped InGaAs using carbontetrabromide by metalorganic molecular beam epitaxy

Auteurs : R. A. Hamm [États-Unis] ; S. Chandrasekhar [États-Unis] ; L. Lunardi [États-Unis] ; M. Geva [États-Unis]

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RBID : ISTEX:31C02A1556E58C074BD507EAC9315CE2D98F8C66

Abstract

Carbon-doped In0.53Ga0.47As structures have been grown on InP by metalorganic molecular beam epitaxy using carbontetrabromide as the dopant source. Hall, secondary ion mass spectrometry (SIMS) and X-ray measurements were done to characterize the material. Doping levels from 2 × 1017 to 7 × 1019 cm−3 were measured with mobilities ranging from 100 to 45 cm2/V · s. SIMS data show very abrupt doping profiles with no apparent memory effects. Hydrogen was measured in the C doped regions, however, no passivation effects were observed and Hall and SIMS data agreed within experimental error. Post-growth anneals of the highest doped samples showed no change in carrier concentration. The incorporation of C showed a strong dependence on the group V beam flux (concentration ∼ flow− 3 4). We believe that this is related to the change in group V vacancy concentration as the group V beam flux is varied. A smaller dependence of C incorporation was also observed with the growth temperature.

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DOI: 10.1016/0022-0248(94)00862-0

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ISTEX:31C02A1556E58C074BD507EAC9315CE2D98F8C66

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<div type="abstract" xml:lang="en">Carbon-doped In0.53Ga0.47As structures have been grown on InP by metalorganic molecular beam epitaxy using carbontetrabromide as the dopant source. Hall, secondary ion mass spectrometry (SIMS) and X-ray measurements were done to characterize the material. Doping levels from 2 × 1017 to 7 × 1019 cm−3 were measured with mobilities ranging from 100 to 45 cm2/V · s. SIMS data show very abrupt doping profiles with no apparent memory effects. Hydrogen was measured in the C doped regions, however, no passivation effects were observed and Hall and SIMS data agreed within experimental error. Post-growth anneals of the highest doped samples showed no change in carrier concentration. The incorporation of C showed a strong dependence on the group V beam flux (concentration ∼ flow− 3 4). We believe that this is related to the change in group V vacancy concentration as the group V beam flux is varied. A smaller dependence of C incorporation was also observed with the growth temperature.</div>
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