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We study a one-dimensional random Kronig-Penney model in the presence of a constant electric field. We rigorously prove for the first time the existence of a transition between a regime of extended states for large field and a regime of power-localized states for small field. There the large-distance behavior of the states is |x|^-α(F) with α(F)~C/F for small field F, confirming a numerical computation of Soukoulis et al.
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Delyon et al. (1984) studied this question.
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