1,256 research outputs found

    Lifespan of solutions for the nonlinear Schr\"odinger equation without gauge invariance

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    We study the lifespan of solutions for the nonlinear Schr\"odinger equation id_{t}u+{\Delta}u={\lambda}|u|^{p}, (t,x)\in[0,T)\timesR^{n}, with the initial condition, where 1<p\leq 1+2/n and {\lambda}\in C. Our main aim in this paper is to prove an upper bound of the lifespan in the subcritical case 1<p<1+2/n.Comment: 10page

    Remark on upper bound for lifespan of solutions to semilinear evolution equations in a two-dimensional exterior domain

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    In this paper we consider the initial-boundary value problem for the heat, damped wave, complex-Ginzburg-Landau and Schr"odinger equations with the power type nonlinearity ∣u∣p|u|^p with pin(1,2]p in (1,2] in a two-dimensional exterior domain. Remark that 2=1+2/N2=1+2/N is well-known as the Fujita exponent. If p>2p>2, then there exists a small global-in-time solution of the damped wave equation for some initial data small enough (see Ikehata'05), and if p<2p<2, then global-in-time solutions cannot exist for any positive initial data (see Ogawa-Takeda'09 and Lai-Yin'17). The result is that for given initial data (f,taug)inH01(Omega)timesL2(Omega)(f,tau g)in H^1_0(Omega)times L^2(Omega) satisfying (f+taug)log∣x∣inL1(Omega)(f+tau g)log |x|in L^1(Omega) with some requirement, the solution blows up at finite time, and moreover, the upper bound for lifespan of solutions to the problem is given as the following {it double exponential type} when p=2p=2: [ lifespan(u) leq exp[exp(Cep^{-1})] . ] The crucial idea is to use test functions which approximates the harmonic function log∣x∣log |x| satisfying Dirichlet boundary condition and the technique for derivation of lifespan estimate in Ikeda-Sobajima(arXiv:1710.06780)

    Life-span of solutions to semilinear wave equation with time-dependent critical damping for specially localized initial data

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    This paper is concerned with the blowup phenomena for initial value problem of semilinear wave equation with critical time-dependent damping term (DW). The result is the sharp upper bound of lifespan of solution with respect to the small parameter \ep when pF(N)≀p≀p0(N+ΞΌ)p_F(N)\leq p\leq p_0(N+\mu), where pF(N)p_F(N) denotes the Fujita exponent for the nonlinear heat equations and p0(n)p_0(n) denotes the Strauss exponent for nonlinear wave equation in nn-dimension with ΞΌ=0\mu=0. Consequently, by connecting the result of D'Abbicco--Lucente--Reissig 2015, our result clarifies the threshold exponent p0(N+ΞΌ)p_0(N+\mu) for dividing blowup phenomena and global existence of small solutions when N=3N=3. The crucial idea is to construct suitable test functions satisfying the conjugate linear equation \pa_t^2\Phi-\Delta \Phi-\pa_t(\frac{\mu}{1+t}\Phi)=0 of (DW) including the Gauss hypergeometric functions; note that the construction of test functions is different from Zhou--Han in 2014.Comment: arXiv admin note: text overlap with arXiv:1709.0440

    Upper bound for lifespan of solutions to certain semilinear parabolic, dispersive and hyperbolic equations via a unified test function method

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    This paper is concerned with the blowup phenomena for initial-boundary value problem for certain semi linear parabolic, dispersive and hyperbolic equations in cone-like domain. The result proposes a unified treatment of estimates for lifespan of solutions to the problem by test function method. The Fujita exponent p=1 + 2/N appears as a threshold of blowup phenomena for small data when CΞ£=RNC_{{\Sigma}}=R^N , but the case of cone-like domain with boundary the threshold changes and explicitly given via the first eigenvalue of corresponding Laplace-Beltrami operator with Dirichlet boundary condition as in Levine-Meier in 1989.Comment: We prove the sharp upper bound of lifespan to semilinear heat equation, damped wave equation and Schr\"odinger equation in the Euclidean space in L^1-setting for convenience of reader

    Life-span of blowup solutions to semilinear wave equation with space-dependent critical damping

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    This paper is concerned with the blowup phenomena for initial value problem of semilinear wave equation with critical space-dependent damping term (DW:VV). The main result of the present paper is to give a solution of the problem and to provide a sharp estimate for lifespan for such a solution when NNβˆ’1<p≀pS(N+V0)\frac{N}{N-1}<p\leq p_S(N+V_0), where pS(N)p_S(N) is the Strauss exponent for (DW:00). The main idea of the proof is due to the technique of test functions for (DW:00) originated by Zhou--Han (2014, MR3169791). Moreover, we find a new threshold value V0=(Nβˆ’1)2N+1V_0=\frac{(N-1)^2}{N+1} for the coefficient of critical and singular damping ∣xβˆ£βˆ’1|x|^{-1}

    Global well-posedness for the semilinear wave equation with time dependent damping in the overdamping case

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    We study global existence of solutions to the Cauchy problem for the wave equation with time-dependent damping and a power nonlinearity in the overdamping case. We prove the global well-posedness for small data in the energy space for the whole energy-subcritical case. This result implies that small data blow-up does not occur in the overdamping case, different from the other cases, i.e. effective or non-effective damping.Comment: 15 pages, typos are corrected and the references are update

    A note on the lifespan of solutions to the semilinear damped wave equation

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    This paper concerns estimates of the lifespan of solutions to the semilinear damped wave equation. We give upper estimates of the lifespan for the semilinear damped wave equation with variable coefficients in all space dimensions.Comment: 9 page

    Global Dynamics below the standing waves for the focusing semilinear Schr\"{o}dinger equation with a repulsive Dirac delta potential

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    We consider the focusing mass supercritical semilinear Schr\"{o}dinger equation with a repulsive Dirac delta potential on the real line (deltaNLS). Our aim in the present paper is to find a necessary and sufficient condition on the data below the standing wave of NLS without a potential to determine the global behavior of the solution. Moreover, we determine the global dynamics of the radial solution whose mass-energy is larger than that of the standing wave and smaller than that of the standing wave of deltaNLS

    The sharp estimate of the lifespan for the semilinear wave equation with time-dependent damping

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    We consider the following semilinear wave equation with time-dependent damping. \begin{align} \tag{NLDW} \left\{ \begin{array}{ll} \partial_t^2 u - \Delta u + b(t)\partial_t u = |u|^{p}, & (t,x) \in [0,T) \times \mathbb{R}^n, \\ u(0,x)=\varepsilon u_0(x), u_t(0,x)=\varepsilon u_1(x), & x \in \mathbb{R}^n, \end{array} \right. \end{align} where n∈Nn \in \mathbb{N}, p>1p>1, Ξ΅>0\varepsilon>0, and b(t)β‰ˆ(t+1)βˆ’Ξ²b(t)\thickapprox (t+1)^{-\beta} with β∈[βˆ’1,1)\beta \in [-1,1). It is known that small data blow-up occurs when 1<p<pF1<p< p_F and, on the other hand, small data global existence holds when p>pFp>p_F, where pF:=1+2/np_F:=1+2/n is the Fujita exponent. The sharp estimate of the lifespan was well studied when 1<p<pF1<p< p_F. In the critical case p=pFp=p_F, the lower estimate of the lifespan was also investigated. Recently, Lai and Zhou obtained the sharp upper estimate of the lifespan when p=pFp=p_F and b(t)=1b(t)=1. In the present paper, we give the sharp upper estimate of the lifespan when p=pFp=p_F and b(t)β‰ˆ(t+1)βˆ’Ξ²b(t)\thickapprox (t+1)^{-\beta} with β∈[βˆ’1,1)\beta \in [-1,1) by the Lai--Zhou method

    Small data blow-up of semi-linear wave equation with scattering dissipation and time-dependent mass

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    In the present paper, we study small data blow-up of the semi-linear wave equation with a scattering dissipation term and a time-dependent mass term from the aspect of wave-like behavior. The Strauss type critical exponent is determined and blow-up results are obtained to both sub-critical and critical cases with corresponding upper bound lifespan estimates. For the sub-critical case, our argument does not rely on the sign condition of dissipation and mass, which gives the extension of the result in \cite{Lai-Sch-Taka18}. Moreover, we show the blow-up result for the critical case which is a new result
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