Abstract

The variation with uniaxial stress of acceptor binding energy, as well as the natural level width, are calculated by the resolvent method in the case of zero-gap structures. We have neglected the warping of the ${\ensuremath{\Gamma}}_{8}$ bands and assumed a short-range impurity potential. When the resonant level merges into the induced gap and becomes a perfectly localized state, an anomaly appears in the stress dependence of the binding energy. A phase-shift analysis of the problem is presented, which enables a complete discussion of the nature of the impurity levels in zero-gap semiconductors.

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