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arXiv · 1606.06980

Suppression of compensating native defect formation during semiconductor processing via excess carriers

Abstract

In many semiconductors, compensating defects set doping limits, decrease carrier mobility, and reduce minority carrier lifetime thus limiting their utility in devices. Native defects are responsible in many cases, but extrinsic dopants may also act as their own compensation when occupying an alternate lattice site. Suppressing the concentrations of compensating defects during processing close to thermal equilibrium is difficult because formation enthalpies are lowered as the Fermi level moves towards the majority band edge. Excess carriers, introduced for example by photogeneration, modify the formation enthalpy of semiconductor defects and thus can be harnessed during crystal growth or annealing to suppress such defect populations. Herein we develop a rigorous and general model for defect formation in the presence of steady-state excess carrier concentrations by combining the standard quasi-chemical formalism with a detailed-balance description that is applicable for any defect state in the bandgap. Considering the quasi-Fermi levels as chemical potentials, we demonstrate that increasing the minority carrier concentration increases the formation enthalpy for typical compensating centers, thus suppressing their formation. This effect is illustrated for the specific example of native GaSb antisite acceptors in nominally un-doped and extrinsically n-type doped GaSb. The model also predicts reductions in the concentration of ionized scattering centers as well as increased mobility. While our treatment is generalized for excess carrier injection or generation in semiconductors by any means, we provide a set of guidelines for applying the concept in photoassisted physical vapor deposition.

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BibTeXRIS

Kirstin Alberi, Michael A. Scarpulla. 2016-06-22. Suppression of compensating native defect formation during semiconductor processing via excess carriers. https://doi.org/10.1038/srep27954

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