低正则强迫项强阻尼波动方程的时变全局吸引子

Pub Date : 2022-12-10 DOI:10.12775/tmna.2022.022
Xinyu Mei, T. Sun, Yongqin Xie, Kaixuan Zhu
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引用次数: 0

摘要

本文基于一个新的时变全局吸引子理论框架(Conti, Pata和Temam \cite{CPT13}),考虑了强阻尼波动方程$\varepsilon(t)u_{tt}-\Delta u_{t}-\Delta u+f(u)=g(x)$,并分别在$\mathcal{H}_{t}=H_{0}^{1}(\Omega)\times L^{2}(\Omega)$和$\mathcal{V}_{t}=H_{0}^{1}(\Omega)\times H_{0}^{1}(\Omega)$中建立了吸引子的存在性。
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Time-dependent global attractors for the strongly damped wave equations with lower regular forcing term
In this paper, based on a new theoretical framework of time-dependent global attractors (Conti, Pata and Temam \cite{CPT13}), we consider the strongly damped wave equations $\varepsilon(t)u_{tt}-\Delta u_{t}-\Delta u+f(u)=g(x)$ and establish the existence of attractors in $\mathcal{H}_{t}=H_{0}^{1}(\Omega)\times L^{2}(\Omega)$ and $\mathcal{V}_{t}=H_{0}^{1}(\Omega)\times H_{0}^{1}(\Omega)$, respectively.
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