<?xml version="1.0" encoding="UTF-8"?>
<OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/"
         xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
         xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd">
<ListRecords>
<oai_dc:dc xmlns="http://www.openarchives.org/OAI/2.0/oai_dc/"
           xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
           xmlns:dc="http://purl.org/dc/elements/1.1/"
           xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
           xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
   	<dc:title>Arnold diffusion in arbitrary degrees of freedom and normally hyperbolic invariant cylinders</dc:title>
   	<dc:creator>Bernard, Patrick</dc:creator>
   	<dc:creator>Kaloshin, Vadim ; https://orcid.org/0000-0002-6051-2628</dc:creator>
   	<dc:creator>Zhang, Ke</dc:creator>
   	<dc:description>We prove a form of Arnold diffusion in the a-priori stable case. Let
H0(p)+ϵH1(θ,p,t),θ∈Tn,p∈Bn,t∈T=R/T,
be a nearly integrable system of arbitrary degrees of freedom n⩾2 with a strictly convex H0. We show that for a “generic” ϵH1, there exists an orbit (θ,p) satisfying
∥p(t)−p(0)∥&gt;l(H1)&gt;0,
where l(H1) is independent of ϵ. The diffusion orbit travels along a codimension-1 resonance, and the only obstruction to our construction is a finite set of additional resonances.

For the proof we use a combination of geometric and variational methods, and manage to adapt tools which have recently been developed in the a-priori unstable case.</dc:description>
   	<dc:publisher>Institut Mittag-Leffler</dc:publisher>
   	<dc:date>2016</dc:date>
   	<dc:type>info:eu-repo/semantics/article</dc:type>
   	<dc:type>doc-type:Article</dc:type>
   	<dc:type>Article</dc:type>
   	<dc:type>http://purl.org/coar/resource_type/c_2df8fbb1</dc:type>
   	<dc:identifier>https://research-explorer.ista.ac.at/record/8494</dc:identifier>
   	<dc:source>Bernard P, Kaloshin V, Zhang K. Arnold diffusion in arbitrary degrees of freedom and normally hyperbolic invariant cylinders. &lt;i&gt;Acta Mathematica&lt;/i&gt;. 2016;217(1):1-79. doi:&lt;a href=&quot;https://doi.org/10.1007/s11511-016-0141-5&quot;&gt;10.1007/s11511-016-0141-5&lt;/a&gt;</dc:source>
   	<dc:language>eng</dc:language>
   	<dc:relation>info:eu-repo/semantics/altIdentifier/doi/10.1007/s11511-016-0141-5</dc:relation>
   	<dc:relation>info:eu-repo/semantics/altIdentifier/issn/0001-5962</dc:relation>
   	<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
</oai_dc:dc>
</ListRecords>
</OAI-PMH>
