<mets:mets OBJID="eprint_4534" LABEL="Eprints Item" xsi:schemaLocation="http://www.loc.gov/METS/ http://www.loc.gov/standards/mets/mets.xsd http://www.loc.gov/mods/v3 http://www.loc.gov/standards/mods/v3/mods-3-3.xsd" xmlns:mets="http://www.loc.gov/METS/" xmlns:mods="http://www.loc.gov/mods/v3" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"><mets:metsHdr CREATEDATE="2020-03-12T11:22:09Z"><mets:agent ROLE="CUSTODIAN" TYPE="ORGANIZATION"><mets:name>WRAP: Warwick Research Archive Portal</mets:name></mets:agent></mets:metsHdr><mets:dmdSec ID="DMD_eprint_4534_mods"><mets:mdWrap MDTYPE="MODS"><mets:xmlData><mods:titleInfo><mods:title>Exponentially small splitting of invariant manifolds near a Hamiltonian-Hopf bifurcation</mods:title></mods:titleInfo><mods:name type="personal"><mods:namePart type="given">José Pedro</mods:namePart><mods:namePart type="family">Gaivão</mods:namePart><mods:role><mods:roleTerm type="text">author</mods:roleTerm></mods:role></mods:name><mods:abstract>Consider an analytic two-degrees of freedom Hamiltonian system with an equilibrium&#13;
point that undergoes a Hamiltonian-Hopf bifurcation, i.e., the eigenvalues of&#13;
the linearized system at the equilibrium change from complex ±β ±iα (α,β &gt; 0) for&#13;
ε &gt; 0 to pure imaginary ±iω1 and ±iω2 (ω1 ≠ ω2 ≠ 0) for ε &lt; 0. At ε = 0 the&#13;
equilibrium has a pair of doubled pure imaginary eigenvalues. Depending on the sign&#13;
of a certain coefficient of the normal form there are two main bifurcation scenarios. In&#13;
one of these (the stable case), two dimensional stable and unstable manifolds of the&#13;
equilibrium shrink and disappear as ε → 0+. At any order of the normal form the stable&#13;
and unstable manifolds coincide and the invariant manifolds are indistinguishable using&#13;
classical perturbation theory. In particular, Melnikov’s method is not capable to evaluate&#13;
the splitting.&#13;
In this thesis we have addressed the problem of measuring the splitting of these&#13;
manifolds for small values of the bifurcation parameter ε. We have estimated the size&#13;
of the splitting which depends on a singular way from the bifurcation parameter. In&#13;
order to measure the splitting we have introduced an homoclinic invariant ωε which&#13;
extends the Lazutkin’s homoclinic invariant defined for area-preserving maps. The main&#13;
result of this thesis is an asymptotic formula for the homoclinic invariant. Assuming&#13;
reversibility, we have proved that there is a symmetric homoclinic orbit such that its&#13;
homoclinic invariant can be estimated as follows,&#13;
ωε = ±2e−πα/2β (ω0 + O(ε1−μ)).&#13;
where μ &gt; 0 is arbitrarily small and ω0 is known as the Stokes constant. This asymptotic&#13;
formula implies that the splitting is exponentially small (with respect to ε). When ω0 ≠ 0&#13;
then the invariant manifolds intersect transversely. The Stokes constant ω0 is defined&#13;
for the Hamiltonian at the moment of bifurcation only. We also prove that it does not&#13;
vanish identically. Finally, we apply our methods to study homoclinic solutions in the&#13;
Swift-Hohenberg equation. Our results show the existence of multi-pulse homoclinic&#13;
solutions and a small scale chaos.</mods:abstract><mods:classification authority="lcc">QA Mathematics</mods:classification><mods:originInfo><mods:dateIssued encoding="iso8061">2010-10</mods:dateIssued></mods:originInfo><mods:originInfo><mods:publisher>University of Warwick;Mathematics Institute</mods:publisher></mods:originInfo><mods:genre>Thesis or Dissertation</mods:genre></mets:xmlData></mets:mdWrap></mets:dmdSec><mets:amdSec ID="TMD_eprint_4534"><mets:rightsMD ID="rights_eprint_4534_mods"><mets:mdWrap MDTYPE="MODS"><mets:xmlData><mods:useAndReproduction>
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