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| Auteurs principaux: | , |
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| Format: | Preprint |
| Publié: |
2014
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| Sujets: | |
| Accès en ligne: | https://arxiv.org/abs/1411.5562 |
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Table des matières:
- In the first part we present a generalized implicit function theorem for abstract equations of the type $F(λ,u)=0$. We suppose that $u_0$ is a solution for $λ=0$ and that $F(λ,\cdot)$ is smooth for all $λ$, but, mainly, we do not suppose that $F(\cdot,u)$ is smooth for all $u$. Even so, we state conditions such that for all $λ\approx 0$ there exists exactly one solution $u \approx u_0$, that $u$ is smooth in a certain abstract sense, and that the data-to-solution map $λ\mapsto u$ is smooth. In the second part we apply the results of the first part to time-periodic solutions of first-order hyperbolic systems of the type $$ \partial_tu_j + a_j(x,λ)\partial_xu_j + b_j(t,x,λ,u) = 0, \; x\in(0,1), \;j=1,\dots,n $$ with reflection boundary conditions and of second-order hyperbolic equations of the type $$ \partial_t^2u-a(x,λ)^2\partial^2_xu+b(t,x,λ,u,\partial_tu,\partial_xu)=0, \; x\in(0,1) $$ with mixed boundary conditions (one Dirichlet and one Neumann). There are at least two distinguishing features of these results in comparison with the corresponding ones for parabolic PDEs: First, one has to prevent small divisors from coming up, and we present explicit sufficient conditions for that in terms of $u_0$ and of the data of the PDEs and of the boundary conditions. And second, in general smooth dependence of the coefficient functions $b_j$ and $b$ on $t$ is needed in order to get smooth dependence of the solution on $λ$, this is completely different to what is known for parabolic PDEs.