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    Maximizers for the Strichartz Inequalities for the Wave Equation

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    We prove the existence of maximizers for Strichartz inequalities for the wave equation in dimensions d3d\geq 3. Our approach follows the scheme given by Shao, which obtains the existence of maximizers in the context of the Schr\"odinger equation. The main tool that we use is the linear profile decomposition for the wave equation which we prove in Rd\mathbb{R}^d, d3d\geq 3, extending the profile decomposition result of Bahouri and Gerard, previously obtained in R3\mathbb{R}^3.Comment: 28 pages, revised version, minor change

    Brane-induced Skyrmions: Baryons in Holographic QCD

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    We study baryons in holographic QCD with D4/D8/D8ˉD4/D8/\bar{D8} multi DD brane system. In holographic QCD, the baryon appears as a topologically non-trivial chiral soliton in a four-dimensional effective theory of mesons, which is called `Brane-induced Skyrmion'. We derive and calculate the Euler-Lagrange equation for the hedgehog configuration with chiral profile F(r)F(r) and ρ\rho-meson profile G~(r)\tilde G(r), and obtain the soliton solution of the holographic QCD.Comment: 5 pages, 6 figure

    Many-Body Theory of Synchronization by Long-Range Interactions

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    Synchronization of coupled oscillators on a dd-dimensional lattice with the power-law coupling G(r)=g0/rαG(r) = g_0/r^\alpha and randomly distributed intrinsic frequency is analyzed. A systematic perturbation theory is developed to calculate the order parameter profile and correlation functions in powers of ϵ=α/d1\epsilon = \alpha/d-1. For αd\alpha \le d, the system exhibits a sharp synchronization transition as described by the conventional mean-field theory. For α>d\alpha > d, the transition is smeared by the quenched disorder, and the macroscopic order parameter \Av\psi decays slowly with g0g_0 as |\Av\psi| \propto g_0^2.Comment: 4 pages, 2 figure

    On Traveling Solitary Waves and Absence of Small Data Scattering for Nonlinear Half-Wave Equations

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    We consider nonlinear half-wave equations with focusing power-type nonlinearity i \pt_t u = \sqrt{-\Delta} \, u - |u|^{p-1} u, \quad \mbox{with $(t,x) \in \R \times \R^d$} with exponents 1<p<1 < p < \infty for d=1d=1 and 1<p<(d+1)/(d1)1 < p < (d+1)/(d-1) for d2d \geq 2. We study traveling solitary waves of the form u(t,x)=eiωtQv(xvt) u(t,x) = e^{i\omega t} Q_v(x-vt) with frequency ωR\omega \in \R, velocity vRdv \in \R^d, and some finite-energy profile QvH1/2(Rd)Q_v \in H^{1/2}(\R^d), Qv≢0Q_v \not \equiv 0. We prove that traveling solitary waves for speeds v1|v| \geq 1 do not exist. Furthermore, we generalize the non-existence result to the square root Klein--Gordon operator \sqrt{-\DD+m^2} and other nonlinearities. As a second main result, we show that small data scattering fails to hold for the focusing half-wave equation in any space dimension. The proof is based on the existence and properties of traveling solitary waves for speeds v<1|v| < 1. Finally, we discuss the energy-critical case when p=(d+1)/(d1)p=(d+1)/(d-1) in dimensions d2d \geq 2.Comment: 17 page
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