The classic example of parametric resonance for ordinary differential equations is a vibrating spring with time varying spring constant This example is studied using Floquet theory. A classic example is κ ( t ) = 1 + ε cos ωt , where one finds regions of instability in the ε , ω plane for which there are solutions which grow exponentially in time. The instability regions are open and with closures touching ε = 0 at critical frequencies (see [ V. Arnold , Ordinary Differential Equations, MIT Press, 1973.], [ W. Magnus and S. Winkler , Hill's equation, Intersc. Tracts Pure Appl. Math. 20, Interscience Publishers John Wiley and Sons, New York-London-Sydney 1966.]). For any t , the constant coefficient problem with κ frozen at κ ( t ) is conservative and has no such growth.
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Requires Authentication UnlicensedSmooth localized parametric resonance for wave equationsLicensedMay 13, 2008
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Requires Authentication UnlicensedEstimates and regularity results for the DiPerna-Lions flowLicensedMay 13, 2008
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Requires Authentication UnlicensedSur le nombre d'éléments exceptionnels d'une base additiveLicensedMay 13, 2008
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Requires Authentication UnlicensedAlder's conjectureLicensedMay 13, 2008
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Requires Authentication UnlicensedLocal monotonicity and mean value formulas for evolving Riemannian manifoldsLicensedMay 13, 2008
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Requires Authentication UnlicensedProjective-injective modules, Serre functors and symmetric algebrasLicensedMay 13, 2008
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Requires Authentication UnlicensedMonodromy of Picard-Fuchs differential equations for Calabi-Yau threefoldsLicensedMay 13, 2008
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Requires Authentication UnlicensedZeros of complex caloric functions and singularities of complex viscous Burgers equationLicensedMay 13, 2008
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Requires Authentication UnlicensedGeneralised form of a conjecture of Jacquet and a local consequenceLicensedMay 13, 2008