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We address the fundamental questions concerning the operator \begin{eqnarray*} H^{\theta_0}\psi(x)=-\psi"(x)+V(x,\omega)\psi(x),,\psi(0)\cos\theta_0-\psi’(0)\sin\theta_0=0. \end{eqnarray*} where the random potential has a variety of forms. In one example, it is composed of width one bumps of random heights where the square root of the heights are in the domain of attraction of a stable law with index or in another it is composed of width one bumps of height one where the distance between bumps is in the domain of attraction of a stable law with index We consider the existence of Lyapunov exponents, integrated density of states and the nature of the spectrum of the operator.

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