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The interaction of an electron with acoustical phonons by the deformation potential is studied with the Feynman path-integral method for zero temperature. An upper bound to the polaron ground-state energy is obtained. The nature of the transition of the quasifree to the self-trapped electron state is discussed for different approximations to the polaron ground-state energy. We find that, within the Feynman approximation, which is the most reliable one for the ground-state energy, there exists a critical value (k₀*) for the cutoff (k₀) in phonon wave-vector space such that for k₀{k}₀*$ (${k}₀$>${k}₀*$) the self-trapping transition is continuous (discontinuous) as a function of the electron-phonon coupling strength.
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Peeters et al. (1985) studied this question.
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