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Motivated by current interest in disordered systems of interacting electrons, the effectiveness of the geometrically averaged density of states, , as an order parameter for the Anderson transition is examined. In the context of finite-size systems we examine complications which arise from finite energy resolution. Furthermore we demonstrate that even in infinite systems a decline in with increasing disorder strength is not uniquely associated with localization.

生成讲解博客的中文版本

生成AI智能校验的中文版本