δ-function-shaped Sb-doping profiles in Si(001) obtained using a low-energy accelerated-ion source during molecular-beam epitaxy

W.-X. Ni, G. V. Hansson, J.-E. Sundgren, L. Hultman, L. R. Wallenberg, J.-Y. Yao, L. C. Markert, and J. E. Greene
Phys. Rev. B 46, 7551 – Published 15 September 1992
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Abstract

Two-dimensional (2D) buried δ-function-shaped Sb-doping profiles have been obtained in Si using a low-energy accelerated Sb-ion source during molecular-beam epitaxy. A combination of secondary-ion mass spectrometry (SIMS), capacitance-voltage (C-V) measurements, and cross-sectional transmission electron microscopy (XTEM) was used to investigate dopant distributions and to determine profile widths. The 2D-sheet Sb-doping concentration NSb, obtained by integrating SIMS δ-doping profiles in samples grown with substrate temperature Ts=620 °C and Sb-ion acceleration potentials VSb=200 and 300 V, was found to vary linearly with the product of the Sb-ion flux and the exposure time (i.e., the ion dose) over the NSb range from 5×1012 to 2×1014 cm2. The full width at half maximum (FWHM) concentration of δ-doping profiles in Si(001) films was less than the depth resolution of both SIMS and C-V measurements (∼10 and 3 nm, respectively). High-resolution XTEM lattice images show that the FWHM was ≤2 nm. This is consistent with dopant incorporation simulations, based upon a multisite transition-state dopant incorporation model, which show that accelerated-beam dopant species are trapped in near-surface substitutional sites with atomic mobilities between those of surface and bulk atoms. Dopant surface segregation during growth is strongly suppressed, and the dopant distribution is determined primarily by the straggle in ion trapping distributions. The present results are compared with profile broadening observed in δ-doped layers obtained by solid-phase epitaxy of amorphous Si containing a buried Sb layer.

  • Received 1 April 1992

DOI:https://doi.org/10.1103/PhysRevB.46.7551

©1992 American Physical Society

Authors & Affiliations

W.-X. Ni, G. V. Hansson, J.-E. Sundgren, and L. Hultman

  • Department of Physics, Linköping University, S-581 83 Linköping, Sweden

L. R. Wallenberg

  • Chemical Center, University of Lund, P.O. Box 124, S-221 00 Lund, Sweden

J.-Y. Yao

  • Department of Physics, Chalmers University of Technology, S-412 96 Göteborg, Sweden

L. C. Markert and J. E. Greene

  • Department of Material Science, The Coordinated Science Laboratory
  • The Materials Research Laboratory, University of Illinois, 1101 West Springfield Avenue, Urbana, Illinois 61801

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Vol. 46, Iss. 12 — 15 September 1992

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