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        <dc:title>A note on micro-instability for Hamiltonian systems close to integrable</dc:title>
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        <bibo:abstract>In this note, we consider the dynamics associated to a perturbation of an integrable Hamiltonian system in action-angle coordinates in any number of degrees of freedom and we prove the following result of ``micro-diffusion&apos;&apos;: under generic assumptions on $ h$ and $ f$, there exists an orbit of the system for which the drift of its action variables is at least of order $ \sqrt {\varepsilon }$, after a time of order $ \sqrt {\varepsilon }^{-1}$. The assumptions, which are essentially minimal, are that there exists a resonant point for $ h$ and that the corresponding averaged perturbation is non-constant. The conclusions, although very weak when compared to usual instability phenomena, are also essentially optimal within this setting.</bibo:abstract>
        <bibo:volume>144</bibo:volume>
        <bibo:issue>4</bibo:issue>
        <bibo:startPage>1553-1560</bibo:startPage>
        <bibo:endPage>1553-1560</bibo:endPage>
        <dc:publisher>American Mathematical Society</dc:publisher>
        <bibo:doi rdf:resource="10.1090/proc/12796" />
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