2012
DOI: 10.1209/0295-5075/100/10006
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Localization-delocalization transition on a separatrix system of nonlinear Schrödinger equation with disorder

Abstract: PACS 05.40.-a -Fluctuation phenomena, random processes, noise, and Brownian motion PACS 05.45.-a -Nonlinear dynamics and chaos PACS 42.25.Dd -Wave propagation in random media Abstract -Localization-delocalization transition in a discrete Anderson nonlinear Schrödinger equation with disorder is shown to be a critical phenomenon − similar to a percolation transition on a disordered lattice, with the nonlinearity parameter thought as the control parameter. In vicinity of the critical point the spreading of the wa… Show more

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Cited by 31 publications
(87 citation statements)
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References 32 publications
(81 reference statements)
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“…Also we predict that the transport of waves at the border of delocalization is subdiffusive, with the exponent α which is inversely proportional with the power nonlinearity increased by one. For quadratic nonlinearity we have (∆n) 2 (t) ∝ t 1/3 for t → +∞ consistently with the previous investigations [10,11]. A kinetic picture of the transport arising from these investigations uses a fractional extension of the diffusion equation to fractional derivatives over the time, signifying non-Markovian dynamics with algebraically decaying time correlations.…”
Section: Discussionsupporting
confidence: 83%
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“…Also we predict that the transport of waves at the border of delocalization is subdiffusive, with the exponent α which is inversely proportional with the power nonlinearity increased by one. For quadratic nonlinearity we have (∆n) 2 (t) ∝ t 1/3 for t → +∞ consistently with the previous investigations [10,11]. A kinetic picture of the transport arising from these investigations uses a fractional extension of the diffusion equation to fractional derivatives over the time, signifying non-Markovian dynamics with algebraically decaying time correlations.…”
Section: Discussionsupporting
confidence: 83%
“…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 analyze delocalization processes as a transport problem for a dynamical system with many coupled degrees of freedom, with an emphasis on the criticality aspects of delocalization. A short account of this approach has been reported previously [20].…”
Section: Introductionmentioning
confidence: 99%