150 research outputs found

    The limiting absorption principle for periodic differential operators and applications to nonlinear Helmholtz equations

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    We prove an LpL^p-version of the limiting absoprtion principle for a class of periodic elliptic differential operators of second order. The result is applied to the construction of nontrivial solutions of nonlinear Helmholtz equations with periodic coefficient functions

    A priori bounds and global bifurcation results for frequency combs modeled by the Lugiato-Lefever equation

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    In nonlinear optics 2Ο€2\pi-periodic solutions a∈C2([0,2Ο€];C)a\in C^2([0,2\pi];\mathbb{C}) of the stationary Lugiato-Lefever equation βˆ’da"=(iβˆ’ΞΆ)a+∣a∣2aβˆ’if-d a"= ({\rm i} -\zeta)a +|a|^2a-{\rm i} f serve as a model for frequency combs, which are optical signals consisting of a superposition of modes with equally spaced frequencies. We prove that nontrivial frequency combs can only be observed for special ranges of values of the forcing and detuning parameters ff and ΞΆ\zeta, as it has been previously documented in experiments and numerical simulations. E.g., if the detuning parameter ΞΆ\zeta is too large then nontrivial frequency combs do not exist, cf. Theorem 2. Additionally, we show that for large ranges of parameter values nontrivial frequency combs may be found on continua which bifurcate from curves of trivial frequency combs. Our results rely on the proof of a priori bounds for the stationary Lugiato-Lefever equation as well as a detailed rigorous bifurcation analysis based on the bifurcation theorems of Crandall-Rabinowitz and Rabinowitz. We use the software packages AUTO and MATLAB to illustrate our results by numerical computations of bifurcation diagrams and of selected solutions

    Bifurcations of nontrivial solutions of a cubic Helmholtz system

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    This paper presents local and global bifurcation results for radially symmetric solutions of the cubic Helmholtz system \begin{equation*} \begin{cases} -\Delta u - \mu u = \left( u^2 + b \: v^2 \right) u &\text{ on } \mathbb{R}^3, \\ -\Delta v - \nu v = \left( v^2 + b \: u^2 \right) v &\text{ on } \mathbb{R}^3. \end{cases} \end{equation*} It is shown that every point along any given branch of radial semitrivial solutions (u0,0,b)(u_0, 0, b) or diagonal solutions (ub,ub,b)(u_b, u_b, b) (for ΞΌ=Ξ½\mu = \nu) is a bifurcation point. Our analysis is based on a detailed investigation of the oscillatory behavior of solutions at infinity that are shown to decay like 1∣x∣\frac{1}{|x|} as ∣xβˆ£β†’βˆž|x|\to\infty.Comment: 31 page

    Dual Variational Methods for a nonlinear Helmholtz system

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    This paper considers a pair of coupled nonlinear Helmholtz equations \begin{align*} -\Delta u - \mu u = a(x) \left( |u|^\frac{p}{2} + b(x) |v|^\frac{p}{2} \right)|u|^{\frac{p}{2} - 2}u, \end{align*} \begin{align*} -\Delta v - \nu v = a(x) \left( |v|^\frac{p}{2} + b(x) |u|^\frac{p}{2} \right)|v|^{\frac{p}{2} - 2}v \end{align*} on RN\mathbb{R}^N where 2(N+1)Nβˆ’1<p<2βˆ—\frac{2(N+1)}{N-1} < p < 2^\ast. The existence of nontrivial strong solutions in W2,p(RN)W^{2, p}(\mathbb{R}^N) is established using dual variational methods. The focus lies on necessary and sufficient conditions on the parameters deciding whether or not both components of such solutions are nontrivial.Comment: Published version. Contains minor revisions: Quote added, explanations on p.12 concerning F_{\mu\nu} = \infty, correction of exponent on p.1
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