On the Aubry-Mather theory for partial differential equations and the stability of stochastically forced ordinary differential equations

dc.contributor.advisorLlave, Rafael de laen
dc.contributor.committeeMemberCaffarelli, Luisen
dc.contributor.committeeMemberKoch, Hansen
dc.contributor.committeeMemberRadin, Charlesen
dc.contributor.committeeMemberRodin, Gregen
dc.contributor.committeeMemberYing, Lexingen
dc.creatorBlass, Timothy Jamesen
dc.date.accessioned2011-06-01T13:51:55Zen
dc.date.accessioned2011-06-01T13:52:06Zen
dc.date.accessioned2017-05-11T22:22:02Z
dc.date.available2011-06-01T13:51:55Zen
dc.date.available2011-06-01T13:52:06Zen
dc.date.available2017-05-11T22:22:02Z
dc.date.issued2011-05en
dc.date.submittedMay 2011en
dc.date.updated2011-06-01T13:52:06Zen
dc.descriptiontexten
dc.description.abstractThis dissertation is organized into four chapters: an introduction followed by three chapters, each based on one of three separate papers. In Chapter 2 we consider gradient descent equations for energy functionals of the type [mathematical equation] where A is a second-order uniformly elliptic operator with smooth coefficients. We consider the gradient descent equation for S, where the gradient is an element of the Sobolev space H[superscipt beta], [beta is an element of](0, 1), with a metric that depends on A and a positive number [gamma] > sup |Vā‚‚ā‚‚|. The main result of Chapter 2 is a weak comparison principle for such a gradient flow. We extend our methods to the case where A is a fractional power of an elliptic operator, and we provide an application to the Aubry-Mather theory for partial differential equations and pseudo-differential equations by finding plane-like minimizers of the energy functional. In Chapter 3 we investigate the differentiability of the minimal average energy associated to the functionals [mathematical equation] using numerical and perturbation methods. We use the Sobolev gradient descent method as a numerical tool to compute solutions of the Euler-Lagrange equations with some periodicity conditions; this is the cell problem in homogenization. We use these solutions to determine the minimal average energy as a function of the slope. We also obtain a representation of the solutions to the Euler-Lagrange equations as a Lindstedt series in the perturbation parameter [epsilon], and use this to confirm our numerical results. Additionally, we prove convergence of the Lindstedt series. In Chapter 4 we present a method for determining the stability of a class of stochastically forced ordinary differential equations, where the forcing term can be obtained by passing white noise through a filter of arbitrarily high degree. We use the Fokker-Planck equation to write a partial differential equation for the second moments, which we turn into an eigenvalue problem for a second-order differential operator. We develop ladder operators to determine analytic expressions for the eigenvalues and eigenfunctions of this differential operator, and thus determine the stability.en
dc.description.departmentMathematicsen
dc.format.mimetypeapplication/pdfen
dc.identifier.urihttp://hdl.handle.net/2152/ETD-UT-2011-05-2798en
dc.language.isoengen
dc.subjectPartial differential equationsen
dc.subjectAubry-Mather theoryen
dc.subjectComparison principleen
dc.subjectLindstedt seriesen
dc.subjectCell problemen
dc.subjectStabilityen
dc.subjectStochastically forced ordinary differential equationsen
dc.titleOn the Aubry-Mather theory for partial differential equations and the stability of stochastically forced ordinary differential equationsen
dc.type.genrethesisen

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