Abstract

We study the localization properties of correlated disordered mixed transmission lines. These systems are formed by the repetition of a set of p successive direct cells followed by q successive dual cells. The spectrum shows a set of d = p + q sub-bands for any kind of disorder where we can find extended and localized states and even gaps. The correlated disorder is introduced only in the capacitances C j , y α , b and inductances L j , y β , b of the dual cells. Meanwhile, the capacitances C j , x and inductances L j , x of the direct cells are kept constant. b measures the amplitude of the disorder, and the correlation exponents α and β quantify the degree of long-range correlation imposed on the system, which is generated by the Fourier filtering method. For fixed p , q and b values it is possible to find extended states as a function of α and β in any of the d sub-bands. For each frequency corresponding to an extended state we can find an asymmetric phase diagram , so that for all α ≥ α c and β ≥ β c with α c ≥ β c , all states are extended. These critical values α c and β c were obtained studying the scaling behavior of the C ω average overlap amplitude. In addition, for fixed α and β , we also find a critical b c value, so for b ≥ b c all states are localized states because the large amplitude b of the fluctuation of the long-range correlated disorder destroys the extended states for all values of α and β . • Mixed transmission lines with p direct cells and q dual cells are studied. • Capacitances an inductances are distributed using two independent sources with long-range correlated disorder. • The localization properties shows an asymmetric phase diagram as a function of the correlation exponent α and β. • The scaling behavior of the C ω average overlap amplitude determines the existence of extended states.

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