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Floquet theory for linear periodic differential equations with discontinuous right-hand side

机译:右侧不连续的线性周期微分方程的Floquet理论

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The Floquet theory for linear periodic differential equations pertains to equations with continuous right-hand side. In the present paper we generalize this theory to systems with discontinuous right-hand side. We assume that in every finite time interval, there are at most a finite number of discontinuities. We demonstrate the applicability of our results in the stability analysis of specific examples.
机译:线性周期微分方程的Floquet理论属于具有连续右手边的方程。在本文中,我们将这一理论推广到具有不连续右手边的系统。我们假设在每个有限的时间间隔内,最多有一定数量的不连续点。我们在具体示例的稳定性分析中证明了我们的结果的适用性。

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