Universal features of self-trapping in nonlinear tight-binding lattices
Author
dc.contributor.author
Bustamante, C.
Author
dc.contributor.author
Molina Gálvez, Mario
Admission date
dc.date.accessioned
2018-12-20T14:28:49Z
Available date
dc.date.available
2018-12-20T14:28:49Z
Publication date
dc.date.issued
2000
Cita de ítem
dc.identifier.citation
Physical Review B - Condensed Matter and Materials Physics, Volumen 62, Issue 23, 2000, Pages 15287-15290
Identifier
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01631829
Identifier
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10.1103/PhysRevB.62.15287
Identifier
dc.identifier.uri
https://repositorio.uchile.cl/handle/2250/156150
Abstract
dc.description.abstract
We use the discrete nonlinear Schrödinger (DNLS) equation to show that nonlinear tight-binding lattices of different geometries and dimensionalities display a universal self-trapping behavior. First, we consider the problem of a single nonlinear impurity embedded in various tight-binding lattices, and calculate the minimum nonlinearity strength to form a stationary bound state. For all lattices, we find that this critical nonlinearity parameter (scaled by the energy of the bound state), in terms of the nonlinearity exponent, falls inside a narrow band, which converges to e1/2 asymptotically. Then, we examine the self-trapping dynamics of an excitation, initially localized on the impurity, and compute the critical nonlinearity parameter for abrupt dynamical self-trapping. For a given nonlinearity exponent, this critical parameter, properly scaled, is found to be nearly the same for all lattices. Same results are obtained when generalizing to completely nonlinear lattices, suggesting an underlying self-trapping universality behavior for all nonlinear ~even disordered! tight-binding lattices described by DNLS