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Attraction property of local center-unstable manifolds for differential equations with state-dependent delay

机译:具有状态依赖时滞的微分方程局部中心不稳定流形的吸引性质

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In the present paper we consider local center-unstable manifolds at a stationary point for a class of functional differential equations of the form $dot{x}(t)=f(x_{t})$ under assumptions that are designed for application to differential equations with state-dependent delay. Here, we show an attraction property of these manifolds. More precisely, we prove that, after fixing some local center-unstable manifold $W_{cu}$ of $dot{x}(t)=f(x_{t})$ at some stationary point $arphi$, each solution of $dot{x}(t)=f(x_{t})$ which exists and remains sufficiently close to $arphi$ for all $tgeq 0$ and which does not belong to $W_{cu}$ converges exponentially for $toinfty$ to a solution on $W_{cu}$.
机译:在本文中,我们针对一类设计为应用的假设,考虑形式为 dot {x}(t)= f(x_ {t})$的一类泛函微分方程在固定点处的局部中心不稳定流形。具有状态相关延迟的微分方程。在这里,我们展示了这些歧管的吸引性质。更确切地说,我们证明,在某个固定点$ varphi $上固定了$ dot {x}(t)= f(x_ {t})$的一些局部中心不稳定流形$ W_ {cu} $之后,每个$ dot {x}(t)= f(x_ {t})$的解,该解对于所有$ t geq 0 $都存在并且足够接近$ varphi $,并且不属于$ W_ {cu}对于$ t to infty $,$以指数形式收敛到$ W_ {cu} $上的解决方案。

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