154 research outputs found

    Stable self-similar blow-up dynamics for slightly L2L^2-supercritical generalized KdV equations

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    In this paper we consider the slightly L2L^2-supercritical gKdV equations ∂tu+(uxx+u∣u∣p−1)x=0\partial_t u+(u_{xx}+u|u|^{p-1})_x=0, with the nonlinearity 5<p<5+ε5<p<5+\varepsilon and 0<ε≪10<\varepsilon\ll 1 . We will prove the existence and stability of a blow-up dynamic with self-similar blow-up rate in the energy space H1H^1 and give a specific description of the formation of the singularity near the blow-up time.Comment: 38 page

    Dynamics of Lattice Kinks

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    In this paper we consider two models of soliton dynamics (the sine Gordon and the \phi^4 equations) on a 1-dimensional lattice. We are interested in particular in the behavior of their kink-like solutions inside the Peierls- Nabarro barrier and its variation as a function of the discreteness parameter. We find explicitly the asymptotic states of the system for any value of the discreteness parameter and the rates of decay of the initial data to these asymptotic states. We show that genuinely periodic solutions are possible and we identify the regimes of the discreteness parameter for which they are expected to persist. We also prove that quasiperiodic solutions cannot exist. Our results are verified by numerical simulations.Comment: 50 pages, 10 figures, LaTeX documen

    Well-posedness and stability results for the Gardner equation

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    In this article we present local well-posedness results in the classical Sobolev space H^s(R) with s > 1/4 for the Cauchy problem of the Gardner equation, overcoming the problem of the loss of the scaling property of this equation. We also cover the energy space H^1(R) where global well-posedness follows from the conservation laws of the system. Moreover, we construct solitons of the Gardner equation explicitly and prove that, under certain conditions, this family is orbitally stable in the energy space.Comment: 1 figure. Accepted for publication in Nonlin.Diff Eq.and App

    A Centre-Stable Manifold for the Focussing Cubic NLS in R1+3R^{1+3}

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    Consider the focussing cubic nonlinear Schr\"odinger equation in R3R^3: iψt+Δψ=−∣ψ∣2ψ. i\psi_t+\Delta\psi = -|\psi|^2 \psi. It admits special solutions of the form eitαϕe^{it\alpha}\phi, where ϕ\phi is a Schwartz function and a positive (ϕ>0\phi>0) solution of −Δϕ+αϕ=ϕ3. -\Delta \phi + \alpha\phi = \phi^3. The space of all such solutions, together with those obtained from them by rescaling and applying phase and Galilean coordinate changes, called standing waves, is the eight-dimensional manifold that consists of functions of the form ei(v⋅+Γ)ϕ(⋅−y,α)e^{i(v \cdot + \Gamma)} \phi(\cdot - y, \alpha). We prove that any solution starting sufficiently close to a standing wave in the Σ=W1,2(R3)∩∣x∣−1L2(R3)\Sigma = W^{1, 2}(R^3) \cap |x|^{-1}L^2(R^3) norm and situated on a certain codimension-one local Lipschitz manifold exists globally in time and converges to a point on the manifold of standing waves. Furthermore, we show that \mc N is invariant under the Hamiltonian flow, locally in time, and is a centre-stable manifold in the sense of Bates, Jones. The proof is based on the modulation method introduced by Soffer and Weinstein for the L2L^2-subcritical case and adapted by Schlag to the L2L^2-supercritical case. An important part of the proof is the Keel-Tao endpoint Strichartz estimate in R3R^3 for the nonselfadjoint Schr\"odinger operator obtained by linearizing around a standing wave solution.Comment: 56 page

    Uniqueness and Nondegeneracy of Ground States for (−Δ)sQ+Q−Qα+1=0(-\Delta)^s Q + Q - Q^{\alpha+1} = 0 in R\mathbb{R}

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    We prove uniqueness of ground state solutions Q=Q(∣x∣)≥0Q = Q(|x|) \geq 0 for the nonlinear equation (−Δ)sQ+Q−Qα+1=0(-\Delta)^s Q + Q - Q^{\alpha+1}= 0 in R\mathbb{R}, where 0<s<10 < s < 1 and 0<α<4s1−2s0 < \alpha < \frac{4s}{1-2s} for s<1/2s < 1/2 and 0<α<∞0 < \alpha < \infty for s≥1/2s \geq 1/2. Here (−Δ)s(-\Delta)^s denotes the fractional Laplacian in one dimension. In particular, we generalize (by completely different techniques) the specific uniqueness result obtained by Amick and Toland for s=1/2s=1/2 and α=1\alpha=1 in [Acta Math., \textbf{167} (1991), 107--126]. As a technical key result in this paper, we show that the associated linearized operator L+=(−Δ)s+1−(α+1)QαL_+ = (-\Delta)^s + 1 - (\alpha+1) Q^\alpha is nondegenerate; i.\,e., its kernel satisfies ker L+=span {Q′}\mathrm{ker}\, L_+ = \mathrm{span}\, \{Q'\}. This result about L+L_+ proves a spectral assumption, which plays a central role for the stability of solitary waves and blowup analysis for nonlinear dispersive PDEs with fractional Laplacians, such as the generalized Benjamin-Ono (BO) and Benjamin-Bona-Mahony (BBM) water wave equations.Comment: 45 page

    Well-Posedness for Semi-Relativistic Hartree Equations of Critical Type

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    We prove local and global well-posedness for semi-relativistic, nonlinear Schr\"odinger equations i∂tu=−Δ+m2u+F(u)i \partial_t u = \sqrt{-\Delta + m^2} u + F(u) with initial data in Hs(R3)H^s(\mathbb{R}^3), s≥1/2s \geq 1/2. Here F(u)F(u) is a critical Hartree nonlinearity that corresponds to Coulomb or Yukawa type self-interactions. For focusing F(u)F(u), which arise in the quantum theory of boson stars, we derive a sufficient condition for global-in-time existence in terms of a solitary wave ground state. Our proof of well-posedness does not rely on Strichartz type estimates, and it enables us to add external potentials of a general class.Comment: 18 pages; replaced with revised version; remark and reference on blow up adde

    On the Dynamics of solitons in the nonlinear Schroedinger equation

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    We study the behavior of the soliton solutions of the equation i((\partial{\psi})/(\partialt))=-(1/(2m)){\Delta}{\psi}+(1/2)W_{{\epsilon}}'({\psi})+V(x){\psi} where W_{{\epsilon}}' is a suitable nonlinear term which is singular for {\epsilon}=0. We use the "strong" nonlinearity to obtain results on existence, shape, stability and dynamics of the soliton. The main result of this paper (Theorem 1) shows that for {\epsilon}\to0 the orbit of our soliton approaches the orbit of a classical particle in a potential V(x).Comment: 29 page

    Stable self similar blow up dynamics for slightly L^2 supercritical NLS equations

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    We consider the focusing nonlinear Schr\"odinger equations i∂tu+Δu+u∣u∣p−1=0i\partial_t u+\Delta u +u|u|^{p-1}=0 in dimension 1≤N≤51\leq N\leq 5 and for slightly L2L^2 supercritical nonlinearities p_c with pc=1+4Np_c=1+\frac{4}{N} and 0<\e\ll 1. We prove the existence and stability in the energy space H1H^1 of a self similar finite time blow up dynamics and provide a qualitative description of the singularity formation near the blow up tim

    Spontaneous Symmetry Breaking in Photonic Lattices: Theory and Experiment

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    We examine an example of spontaneous symmetry breaking in a double-well waveguide with a symmetric potential. The ground state of the system beyond a critical power becomes asymmetric. The effect is illustrated numerically, and quantitatively analyzed via a Galerkin truncation that clearly shows the bifurcation from a symmetric to an asymmetric steady state. This phenomenon is also demonstrated experimentally when a probe beam is launched appropriately into an optically induced photonic lattice in a photorefractive material.Comment: 4 pages, 3 figure
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