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Quasi-periodic solutions of nonlinear wave equations with quasi-periodic forcing

机译:具有准周期强迫的非线性波动方程的准周期解

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This work focuses on one-dimensional (1D) quasi-periodically forced nonlinear wave equations. This means studying u(u) - u(xx) + mu u + epsilon phi(t)h(u) = 0, mu > 0, with Dirichlet boundary conditions, where epsilon is a small positive parameter, phi(t) is a real analytic quasi-periodic function in t with frequency vector omega = (omega(1), omega(2) ..., omega(m)) and the nonlinearity h is a real analytic odd function of the form h(u) = eta(1)u + eta(2 (r) over bar +1)u(2 (r) over bar +1) + Sigma(k >=(r) over bar1) eta(2k+1)u(2k+1), eta(1), eta(2 (r) over bar +1) not equal 0, (r) over bar is an element of N. It is shown that, under a suitable hypothesis on phi(t) and h, there are many quasi-periodic solutions for the above equation via KAM theory.
机译:这项工作集中于一维(1D)准周期强迫非线性波动方程。这意味着在Dirichlet边界条件下研究u(u)-u(xx)+ mu u + epsilon phi(t)h(u)= 0,mu> 0,其中epsilon是一个小的正参数,phi(t)为频率向量为omega =(omega(1),omega(2)...,omega(m))的t中的实解析准周期函数,并且非线性h为h(u)形式的实解析奇函数= eta(1)u + eta(2(r)超过小节+1)u(2(r)超过小节+1)+ Sigma(k> =(r)超过bar1)eta(2k + 1)u(2k +1),eta(1),棒(+1)上的eta(2(r)不等于0,棒上的(r)是N的元素。证明了在关于phi(t)和h,通过KAM理论,上述方程有许多准周期解。

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