Quasi-periodic solutions for p-Laplacian equations with jumping nonlinearity and unbounded potential terms

preprint2013arXivOpen access

Abstract

In this paper, we are concerned with the boundedness of all the solutions for a kind of second order differential equations with p-Laplacian term (ϕp(x′))′+aϕp(x+)−bϕp(x−)+f(x)=e(t)(ϕ_p(x'))'+aϕ_p(x^+)-bϕ_p(x^-)+f(x)=e(t), where x+=max⁡(x,0)x^+=\max (x,0), x−=max⁡(−x,0)x^- =\max(-x,0), ϕp(s)=∣s∣p−2sϕ_p(s)=|s|^{p-2}s, p≥2p\geq2, aa and bb are positive constants (a≠b)(a\not=b), and satisfy 1a1p+1b1p=2ω−1\frac{1}{a^{\frac{1}{p}}}+\frac{1}{b^{\frac{1}{p}}}=2ω^{-1} ,where $ω\in \RR^+ \backslash \QQ$, the perturbation ff is unbounded, e(t)∈C6e(t)\in {\cal C}^{6} is is a smooth 2πp2π_p-periodic function on tt, where πp=2π(p−1)1ppsin⁡πpπ_p=\frac{2π(p-1)^{\frac{1}{p}}}{p\sin\fracπ{p}}.

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