Abstract
In this paper, we consider the second KdV equation with the external parameters
under zero mean-value periodic boundary conditions
where \(M_\sigma \) is a real Fourier multiplier. It is proved that the equations admit a Whitney smooth family of small amplitude, real analytic almost periodic solutions with all frequencies. The proof is based on a conserved quantity \(\int _0^{2\pi } u^2 dx\), Töplitz–Lipschitz property of the perturbation and an abstract infinite dimensional KAM theorem. By taking advantage of the conserved quantity \(\int _0^{2\pi } u^2 dx\) and Töplitz–Lipschitz property of the perturbation, our normal form part is independent of angle variables in spite of the unbounded perturbation. This is the first attempt to prove the almost periodic solutions for the unbounded perturbation case.
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Notes
The norm \(\Vert \cdot \Vert _{D_\rho ( r,s), \mathcal O}\) for scalar functions is defined in (2.3). The vector function \(G: D_\rho ( r,s)\times \mathcal{O}\rightarrow {\mathbb C}^m\), (\(m<\infty \)) is similarly defined as \(\Vert G\Vert _{D_\rho ( r,s), \mathcal O}=\sum \nolimits _{i=1}^m\Vert G_i\Vert _{D_\rho ( r,s), \mathcal O}\).
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Acknowledgments
We would like to thank Yingfei Yi and Jiangong You for fruitful discussions about this work. We would also like to thank the anonymous referee for good suggestions and pointing out some mistakes in the former version. This work is partially supported by NSFC Grant 11271180. This work is also partially supported by a Project Funded by the Priority Academic Program Development of Jiangsu Higher Education Institutions.
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Appendix
Appendix
Lemma 6.5
If
then
In particular, if \(\eta \sim \varepsilon ^{\frac{1}{3}}\), \(\varepsilon ', \varepsilon ''\sim \varepsilon \), we have \(\Vert X_{\{F,G\}}\Vert _{D_\rho (r-\sigma ,\eta s),\mathcal O}\sim \varepsilon ^{\frac{4}{3}}\).
For the proof, see [18]. \(\square \)
Let V be an open domain in a real Banach space E with norm\(\Vert \cdot \Vert \), B a subset of another real Banach space, and \(X:V\times B\rightarrow E\) a parameter dependent vector field on V, which is \(C^{1}\) on V and Lipschitz on B. Let \(\phi ^{t}\) be its flow. Suppose there is a subdomain \(U\subset V\) such that \(\phi ^{t} :U\times B\rightarrow V\) for \(-1\le t\le 1\).
Lemma 6.6
Under the preceding assumptions,
For the proof, see [35]. \(\square \)
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Geng, J., Hong, W. Invariant Tori of Full Dimension for Second KdV Equations with the External Parameters. J Dyn Diff Equat 29, 1325–1354 (2017). https://doi.org/10.1007/s10884-015-9505-3
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DOI: https://doi.org/10.1007/s10884-015-9505-3