Titlebook: Anderson Localization and Its Ramifications; Disorder, Phase Cohe Tobias Brandes,S. Kettemann Book 2003 Springer-Verlag Berlin Heidelberg 2

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Drug Epidemiology / Pharmako-Epidemiologiely strong disorder can give rise to a transition of the transport properties from conducting behavior with finite resistance . to insulating behavior with .=∞ as .→0 as was pointed out by Anderson in 1958 [4]. This phenomenon is called the disorder-driven metal-insulator transition (MIT) [3, 1, 4] a

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https://doi.org/10.1007/978-1-4899-2587-9on (MIT) in particular, the transfer matrix has proved the most productive. In this chapter I will present several related approaches that might broadly be considered as . methods. As a definition of a transfer matrix we may consider: “An operator which uses a set of quantities defined at one positi

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Andrea B. MacNeill,Jacobus Lubsens for this new type of laser include strongly disordered semiconductors [1, 2], polymer systems [3], solutions of .. nanoparticles [4, 5], as well as synthetic opals infiltrated with laser dyes [6]. The feedback in random lasers is provided by the random scattering of light in a dielectric with a sp

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Drug Evaluation in Angina Pectorist propagation in a medium with fluctuating dielectric constant. Consider, for concreteness, a two-dimensional geometry (quantum well for an electron and a thin film for light). Then both equations can be presented in the form . where ρ is the in-plane coordinate. For an electron with mass . and ener

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Developments in Cardiovascular Medicinen semiconductors consider nanostructures, where at least one characteristic system dimension is on the nanometer scale. Your judgment whether this provocative statement actually is true or not will depend on how broadly you define the terms . and .. But doubtlessly, the enormous economic impact of s