Abstract
In this chapter, we will consider again the periodic problem
where \(g: [0,T] \times \mathbb{R} \rightarrow \mathbb{R}\) is a continuous function, and we will concentrate in finding sufficient conditions for the existence of a solution in the case when
where \(\lambda _{N} = \left (\frac{2\pi N} {T} \right )^{2}\) is an eigenvalue of the differential operator, and h is a bounded function.
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Notes
- 1.
The notation o(ɛ) used here has the following meaning: for some function R(ɛ; θ0 ),
$$\displaystyle{ R(\varepsilon;\theta _{0}) = o(\varepsilon )\quad \Longleftrightarrow\quad \lim _{\varepsilon \rightarrow 0^{+}} \frac{1} {\varepsilon } R(\varepsilon;\theta _{0}) = 0\,,\quad \mbox{ uniformly in }\theta _{0} \in [0,\tau ]. }$$
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Fonda, A. (2016). Playing Around Resonance. In: Playing Around Resonance. Birkhäuser Advanced Texts Basler Lehrbücher. Birkhäuser, Cham. https://doi.org/10.1007/978-3-319-47090-0_6
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