1991
DOI: 10.1007/bf02099674
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Perturbation theory for periodic orbits in a class of infinite dimensional Hamiltonian systems

Abstract: We consider a class of Hamiltonian systems describing an infinite array of coupled anharmonic oscillators, and we study the bifurcation of periodic orbits off the equilibrium point. The family of orbits we construct can be parametrized by their periods which belong to Cantor sets of large measure containing certain periods of the linearized problem as accumulation points. The infinitely many holes forming a dense set on which the existence of a periodic orbit cannot be proven originate from a dense set of reso… Show more

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Cited by 36 publications
(40 citation statements)
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“…Another intriguing question is the relation between time-periodic and spatially localized solutions in nonlinear disordered lattices [7,366,219,14,221,220,197] and the diffusion of an initially localized excitation [367,283]. This is currently an active field of research, and we can expect to receive fresh news in the very near future.…”
Section: Q-breathers Localization In Normal Mode Space and The Fermmentioning
confidence: 97%
See 1 more Smart Citation
“…Another intriguing question is the relation between time-periodic and spatially localized solutions in nonlinear disordered lattices [7,366,219,14,221,220,197] and the diffusion of an initially localized excitation [367,283]. This is currently an active field of research, and we can expect to receive fresh news in the very near future.…”
Section: Q-breathers Localization In Normal Mode Space and The Fermmentioning
confidence: 97%
“…Typical propagation distances in waveguide arrays are rather short, so that usually the effects of light dispersion in each individual waveguide are neglected. 7 Under this assumption, the total field distribution in a one-dimensional waveguide array, see Fig. 63, can be approximated as the superposition of linear waveguide modes of each individual waveguide E(x, z) = n E n (z)ψ n (x) exp(−iλ 0 z), (10.9) where ψ n (x) ≡ ψ 0 (x − nd), ψ 0 (x) is the linear waveguide mode with corresponding propagation constant λ 0 :…”
Section: Basic Principles and Modelingmentioning
confidence: 97%
“…¿From a mathematical point of view, Albanese and Fröhlich have proved the existence of breathers for a class of random Hamiltonian systems describing an infinite array of coupled anharmonic oscillators [AF91] (see also the earlier work [FSW86] of Fröhlich et al concerning quasiperiodic localized oscillations). These breather families can be parametrized by the solutions frequencies, which belong to fat Cantor sets (i.e.…”
Section: Introductionmentioning
confidence: 99%
“…(By contrast, simple periodic solutions may remain localized, forming intrinsic localized modes ("discrete breathers") which may be dynamical attractors for some initial conditions [6].) However, these arguments do not hold when the linear spectrum is purely discrete, and it is known, e.g., that spatially localized periodic solutions with frequencies inside the linear spectrum exist generically in systems with linear Anderson localization [7,8].…”
mentioning
confidence: 99%