Electron diffusion length and escape probability measurements for <i>p</i>-type GaAs(100) epitaxies

  • G. Vergara
    Departamento de Física Aplicada, Centro de Investigación y Desarrollo de la Armada (CIDA), Arturo Soria 289, 28033-Madrid
  • L. J. Gómez
    Departamento de Física Aplicada, Centro de Investigación y Desarrollo de la Armada (CIDA), Arturo Soria 289, 28033-Madrid
  • J. Presa
    Departamento de Física Aplicada, Centro de Investigación y Desarrollo de la Armada (CIDA), Arturo Soria 289, 28033-Madrid
  • M. T. Montojo
    Departamento de Física Aplicada, Centro de Investigación y Desarrollo de la Armada (CIDA), Arturo Soria 289, 28033-Madrid

抄録

<jats:p>According to the two-minima electron diffusion model of Spicer, James, and Moll [W. E. Spicer, Quant. Rep. 9, April (1968); L. W. James and Z. L. Moll, Phys. Rev. 183, 740 (1969)] for near threshold photoemission, minority-carrier diffusion length L and escape probability P for a variety of Beryllium doped GaAs(100) epitaxies grown by molecular beam epitaxy, have been obtained. These epitaxies, before being activated with cesium and oxygen by using the two-stages method described by Stocker and Goldstein [B. J. Stocker, Surf. Sci. 47, 501 (1975); B. Goldstein, ibid. 47, 143 (1975)], were passivated in two different ways. (i) Chemically, with a 5:1:1 H2O:H2O2:H2SO4 solution and (ii) by the deposition of a 700–800 Å thick antimony layer. A better performance of the samples using this last type of passivation is shown. In order to evaluate L and P from the electron diffusion model, it is necessary to know the dispersion relation of the absorption coefficient for each sample. They have been obtained from normal-incidence reflectance measurements by means of a Kramers–Krönig analysis. The electronic diffusion length values obtained ranged from 4.5 to 2.1 μm and the escape probabilities between 8.1% and 20.2% for Be concentrations of 1×1018 and 1×1019 cm−3, respectively.</jats:p>

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