503 research outputs found

    Asymptotic profiles for a nonlinear Kirchhoff equation with combined powers nonlinearity

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    We study asymptotic behavior of positive ground state solutions of the nonlinear Kirchhoff equation βˆ’(a+b∫RNβˆ£βˆ‡u∣2)Ξ”u+Ξ»u=uqβˆ’1+upβˆ’1inΒ RN, -\Big(a+b\int_{\mathbb R^N}|\nabla u|^2\Big)\Delta u+ \lambda u= u^{q-1}+ u^{p-1} \quad {\rm in} \ \mathbb R^N, as Ξ»β†’0\lambda\to 0 and Ξ»β†’+∞\lambda\to +\infty, where N=3N=3 or N=4N= 4, 2<q≀p≀2βˆ—2<q\le p\le 2^*, 2βˆ—=2NNβˆ’22^*=\frac{2N}{N-2} is the Sobolev critical exponent, a>0a>0, bβ‰₯0b\ge 0 are constants and Ξ»>0\lambda>0 is a parameter. In particular, we prove that in the case 2<q<p=2βˆ—2<q<p=2^*, as Ξ»β†’0\lambda\to 0, after a suitable rescaling the ground state solutions of the problem converge to the unique positive solution of the equation βˆ’Ξ”u+u=uqβˆ’1-\Delta u+u=u^{q-1} and as Ξ»β†’+∞\lambda\to +\infty, after another rescaling the ground state solutions of the problem converge to a particular solution of the critical Emden-Fowler equation βˆ’Ξ”u=u2βˆ—βˆ’1-\Delta u=u^{2^*-1}. We establish a sharp asymptotic characterisation of such rescalings, which depends in a non-trivial way on the space dimension N=3N=3 and N=4N= 4. We also discuss a connection of our results with a mass constrained problem associated to the Kirchhoff equation with the mass normalization constraint ∫RN∣u∣2=c2\int_{\mathbb R^N}|u|^2=c^2.Comment: 40 page

    Multiple Solutions for the Asymptotically Linear Kirchhoff Type Equations on R

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    The multiplicity of positive solutions for Kirchhoff type equations depending on a nonnegative parameter Ξ» on RN is proved by using variational method. We will show that if the nonlinearities are asymptotically linear at infinity and Ξ»>0 is sufficiently small, the Kirchhoff type equations have at least two positive solutions. For the perturbed problem, we give the result of existence of three positive solutions

    Normalized Solutions to Nonautonomous Kirchhoff Equation

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    In this paper, we study the existence of normalized solutions to the following Kirchhoff equation with a perturbation: {βˆ’(a+b∫RNβˆ£βˆ‡u∣2dx)Ξ”u+Ξ»u=∣u∣pβˆ’2u+h(x)∣u∣qβˆ’2u,Β inΒ RN,∫RN∣u∣2dx=c,u∈H1(RN), \left\{ \begin{aligned} &-\left(a+b\int _{\mathbb{R}^{N}}\left | \nabla u \right|^{2} dx\right)\Delta u+\lambda u=|u|^{p-2} u+h(x)\left |u\right |^{q-2}u, \quad \text{ in } \mathbb{R}^{N}, \\ &\int_{\mathbb{R}^{N}}\left|u\right|^{2}dx=c, \quad u \in H^{1}(\mathbb{R}^{N}), \end{aligned} \right. where 1≀N≀3,a,b,c>0,1≀q<21\le N\le 3, a,b,c>0, 1\leq q<2, λ∈R\lambda \in \mathbb{R}. We treat three cases. (i)When 2<p<2+4N,h(x)β‰₯02<p<2+\frac{4}{N},h(x)\ge0, we obtain the existence of global constraint minimizers. (ii)When 2+8N<p<2βˆ—,h(x)β‰₯02+\frac{8}{N}<p<2^{*},h(x)\ge0, we prove the existence of mountain pass solution. (iii)When 2+8N<p<2βˆ—,h(x)≀02+\frac{8}{N}<p<2^{*},h(x)\leq0, we establish the existence of bound state solutions.Comment: arXiv admin note: text overlap with arXiv:2301.07926 by other author
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