1997
DOI: 10.1007/978-1-4615-5835-4_9
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Intrinsic Localized Modes in Anharmonic Lattices

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Cited by 3 publications
(3 citation statements)
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“…For a classical nonlinear oscillator array, there are a number of characteristic ILM properties, probed theoretically, such as their interaction with an ac driver, 14,34 -36 their propagation 5,[37][38][39][40] and amplitude dependent mobility 4,6,[40][41][42] in a discrete lattice potential, 43,44 as well as their interactions with impurities, [45][46][47][48][49][50] that still need to be examined experimentally. Note that strongly excited ILMs 42 can be trapped anywhere in the lattice, so they also could approach impurity mode behavior.…”
Section: Introductionmentioning
confidence: 99%
“…For a classical nonlinear oscillator array, there are a number of characteristic ILM properties, probed theoretically, such as their interaction with an ac driver, 14,34 -36 their propagation 5,[37][38][39][40] and amplitude dependent mobility 4,6,[40][41][42] in a discrete lattice potential, 43,44 as well as their interactions with impurities, [45][46][47][48][49][50] that still need to be examined experimentally. Note that strongly excited ILMs 42 can be trapped anywhere in the lattice, so they also could approach impurity mode behavior.…”
Section: Introductionmentioning
confidence: 99%
“…(12) has long been studied in the context of FPU lattice theory. Following earlier pioneering works Page, 1990] (also see in [Kiselev et al, 1995;Bickham et al, 1997] and Refs. therein), the existence of DBs in FPU chains was rigorously proven in [James, 2001]; see in [Sánchez-Rey et al, 2004;Flach & Gorbach, 2004] for two recent studies, establishing the existence of bright and dark breathers in FPU chains.…”
Section: Discrete Localized Oscillations In the Longitudinal Directionmentioning
confidence: 95%
“…Following the pioneering analytical and numerical considerations of ILM existence due to coupling anharmonicity (in discrete FPU chains) by Sievers, Takeno, Page and coworkers [Sievers & Takeno, 1988;Page, 1990] presented in the late 1980's (also see [Kiselev et al, 1995;Bickham et al, 1997] for a review), the existence of DB modes has been rigorously proven in the past, for a wide class of nonlinear discrete lattices. Two main axes of proof have been suggested so far, namely: (i) the analytic continuation from the uncoupled ("anti-continuous") limit to a weakly interacting oscillator chain [MacKay & Aubry, 1994;Aubry, 1997], and (ii) the relation of DB existence to (intersection points of) the homoclinic orbits in the phase space defined by the Fourier component amplitudes {A nk } [Flach, 1995] (also see [Bountis, 2000]).…”
Section: Intrinsic Localized Modesmentioning
confidence: 99%