2017
DOI: 10.1140/epjd/e2017-80057-2
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A bifurcation analysis for the Lugiato-Lefever equation

Abstract: The Lugiato-Lefever equation is a cubic nonlinear Schrödinger equation, including damping, detuning and driving, which arises as a model in nonlinear optics. We study the existence of stationary waves which are found as solutions of a four-dimensional reversible dynamical system in which the evolutionary variable is the space variable. Relying upon tools from bifurcation theory and normal forms theory, we discuss the codimension 1 bifurcations. We prove the existence of various types of steady solutions, inclu… Show more

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Cited by 26 publications
(29 citation statements)
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“…In terms of spatial dynamics this point corresponds to a reversible Takens-Bogdanov bifurcation [51,55], and a weakly nonlinear solution of the form A − A + ∼ asech 2 (bx) can be obtained as already done in Refs. [64][65][66].…”
Section: Bifurcation Structure Of Type-i Localized Statesmentioning
confidence: 99%
“…In terms of spatial dynamics this point corresponds to a reversible Takens-Bogdanov bifurcation [51,55], and a weakly nonlinear solution of the form A − A + ∼ asech 2 (bx) can be obtained as already done in Refs. [64][65][66].…”
Section: Bifurcation Structure Of Type-i Localized Statesmentioning
confidence: 99%
“…Unlike [8,9] we consider (1.1) on certain spaces of 2π-periodic functions. We obtain a very rich bifurcation picture which is not limited to local considerations as in [8,9,20]. In Theorem 1 and Theorem 2 we find a priori bounds and uniqueness results which allow us to show that (a) nonconstant solutions of (1.1) only occur in the range sign(d)ζ ∈ [ζ * , ζ * ], (b) nonconstant solutions of (1.1) satisfy a ∞ + |ζ| ≤ C. Here, the values ζ * , ζ * and C are explicit and only depend on the parameters f, d. We begin with our results concerning pointwise a priori bounds for solutions of (1.1) in terms of the parameters ζ, d, f .…”
Section: Introductionmentioning
confidence: 99%
“…The case d < 0 corresponds to normal dispersion whereas d > 0 is called the anomalous regime, cf. [8,9]. The loss of power due to radiation and waveguide coupling is modeled by the damping term −iâ k (t).…”
Section: Introductionmentioning
confidence: 99%
“…We expect these results to provide a deeper understanding of the dynamics of many other dissipative structures in WGM resonators [40,41]. In the light of previous research works that already unveiled key mathematical properties of the LLE equation [42][43][44][45], we also expect our analysis to lead the way to a stability enhancement of these patterns, for the benefit of the many targeted applications [4][5][6][7][8][9].…”
mentioning
confidence: 59%