2014
DOI: 10.1103/physreve.89.062921
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Topological approximation of the nonlinear Anderson model

Abstract: We study the phenomena of Anderson localization in the presence of nonlinear interaction on a lattice. A class of nonlinear Schrödinger models with arbitrary power nonlinearity is analyzed. We conceive the various regimes of behavior, depending on the topology of resonance-overlap in phase space, ranging from a fully developed chaos involving Lévy flights to pseudochaotic dynamics at the onset of delocalization. It is demonstrated that the quadratic nonlinearity plays a dynamically very distinguished role in t… Show more

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Cited by 21 publications
(78 citation statements)
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“…We reiterate that non-diagonal elements V k,m1,m2,m3 characterize couplings between each four eigenstates with wave numbers k, m 1 , m 2 , and m 3 . The comprehension of Hamiltonian character of the dynamics paves the way for a consistency analysis of the various transport scenarios behind the Anderson localization problem (with the topology of resonance overlap taken into account) [10,11]. To this end, the transport problem for the wave function becomes essentially a topological problem in phase space.…”
Section: The Three-step Topological Approachmentioning
confidence: 99%
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“…We reiterate that non-diagonal elements V k,m1,m2,m3 characterize couplings between each four eigenstates with wave numbers k, m 1 , m 2 , and m 3 . The comprehension of Hamiltonian character of the dynamics paves the way for a consistency analysis of the various transport scenarios behind the Anderson localization problem (with the topology of resonance overlap taken into account) [10,11]. To this end, the transport problem for the wave function becomes essentially a topological problem in phase space.…”
Section: The Three-step Topological Approachmentioning
confidence: 99%
“…Then the percolation transition threshold can be translated into a critical value of the nonlinearity control parameter, such that above this value the field spreads to infinity, and is dynamically localized in spite of these nonlinearities otherwise. This critical value when account is taken for hierarchical geometry of the Cayley tree is found to be β c = 1/ ln 2 ≈ 1.4427 [10,11], a fancy number representing the topology of nonlinear interaction posed by the quadratic power term. It was argued based on a random walk approach that in vicinity of the criticality the spreading of the wave field is subdiffusive in the limit t → +∞, and that the second moments grow with time as a power law…”
Section: Introductionmentioning
confidence: 99%
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