2006
DOI: 10.1017/s001708950600317x
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Global Existence in Infinite Lattices of Nonlinear Oscillators: The Discrete Klein-Gordon Equation

Abstract: Abstract. Pointing out the difference between the Discrete Nonlinear Schrödinger equation with the classical power law nonlinearity -for which solutions exist globally, independently of the sign and the degree of the nonlinearity, the size of the initial data and the dimension of the lattice -we prove either global existence or nonexistence, in time, for the Discrete Klein-Gordon equation with the same type of nonlinearity (but of "blow-up" sign), under suitable conditions on the initial data, and sometimes on… Show more

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Cited by 5 publications
(10 citation statements)
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“…If µ is a Floquet multiplier, then the corresponding Floquet exponent λ (which is unique modulo 2πi/T ) is related to µ by µ = e λT . For every Floquet exponent λ, there is a corresponding solution v(t) = e λt w(t) to the linearized equation (7), where w(t) is periodic with period T (see, for example, [50,Lemma 2.1.29]). Substituting this ansatz into (7), we obtain the Floquet eigenvalue problem…”
Section: Mathematical Backgroundmentioning
confidence: 99%
See 2 more Smart Citations
“…If µ is a Floquet multiplier, then the corresponding Floquet exponent λ (which is unique modulo 2πi/T ) is related to µ by µ = e λT . For every Floquet exponent λ, there is a corresponding solution v(t) = e λt w(t) to the linearized equation (7), where w(t) is periodic with period T (see, for example, [50,Lemma 2.1.29]). Substituting this ansatz into (7), we obtain the Floquet eigenvalue problem…”
Section: Mathematical Backgroundmentioning
confidence: 99%
“…For every Floquet exponent λ, there is a corresponding solution v(t) = e λt w(t) to the linearized equation (7), where w(t) is periodic with period T (see, for example, [50,Lemma 2.1.29]). Substituting this ansatz into (7), we obtain the Floquet eigenvalue problem…”
Section: Mathematical Backgroundmentioning
confidence: 99%
See 1 more Smart Citation
“…which describes the dynamics of an infinitely long, one-dimensional lattice of particles. The quantity u n represents the displacement of the nth particle in the integer lattice as a function of the time t. Each particle is harmonically coupled to its two nearest neighbors via the discrete second difference operator Δ 2 , and the strength of this coupling is quantified by the parameter d. The particles are subject to an external, nonlinear, on-site potential V(u), such that f (u) = V (u), which can be of different type depending on the model [7,8]. Common nonlinearities are shown in table 1.…”
Section: Introductionmentioning
confidence: 99%
“…describes the dynamics of an infinitely long, one-dimensional lattice of particles which are harmonically coupled to their neighbors through the discrete second difference operator ∆ 2 and are subject to an external, nonlinear, on-site potential P (u) such that f (u) = P ′ (u) [8].…”
Section: Introductionmentioning
confidence: 99%