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<p class="MsoNormal"><span lang="EN-US">Dear all,<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="EN-US"><o:p> </o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">The starting time of Valerio Assenza’s talk next Tuesday has been moved to
<b>3:30pm</b> (i.e. thirty minutes later than the original time) so that some more interested people can come.
<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="EN-US"><o:p> </o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">Have a great day!<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="EN-US"><o:p> </o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">Gabriele<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="en-NL"><o:p> </o:p></span></p>
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<p class="MsoNormal"><b><span lang="EN-US" style="mso-fareast-language:#2000">From:</span></b><span lang="EN-US" style="mso-fareast-language:#2000"> _list_topology.beta-bounces <topology.beta-bounces@listserver.vu.nl>
<b>On Behalf Of </b>Benedetti, G. (Gabriele)<br>
<b>Sent:</b> Tuesday, 20 September 2022 18:51<br>
<b>To:</b> _list_topology.beta <topology.beta@listserver.vu.nl><br>
<b>Subject:</b> [Topology.beta] Announcement: Talk by Valerio Assenza<o:p></o:p></span></p>
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<p class="MsoNormal"><o:p> </o:p></p>
<p class="MsoNormal"><span lang="DE">Dear all,<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="DE"><o:p> </o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">Valerio Assenza from the University of Heidelberg will give a talk<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">On Tuesday October 4, at 3pm in the MathLab.<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">Below you find the title and abstract. <o:p>
</o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">Starting from 17:30 we will have drinks at Deboele bar and then move to Market 33 for dinner.<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="EN-US"><o:p> </o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">Hope to see many of you there!<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="EN-US"><o:p> </o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">Best wishes,<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="EN-US"><o:p> </o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">Gabriele<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="EN-US"><o:p> </o:p></span></p>
<p class="MsoNormal"><span lang="EN-US">Title:<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="en-NL">Magnetic Curvature and Existence of Closed Magnetic Geodesic<o:p></o:p></span></p>
<p class="MsoPlainText"><span lang="en-NL"><o:p> </o:p></span></p>
<p class="MsoPlainText"><span lang="en-NL">Abstract: <o:p></o:p></span></p>
<p class="MsoPlainText"><span lang="en-NL">A Magnetic System is the toy model for the motion of a charged particle moving on a Riemannian Manifold endowed with a magnetic field.
<o:p></o:p></span></p>
<p class="MsoNormal"><span lang="en-NL">Solutions for such systems are called Magnetic Geodesic and preserve the Kinetic Energy. One of the most relevant investigative interest in the theory is to understand the existence and in case the topological nature
of Closed Magnetic Geodesic</span><span lang="EN-US">s</span><span lang="en-NL"> (periodic solution</span><span lang="EN-US">s</span><span lang="en-NL">) in a given level of the energy. I will introduce the Magnetic Curvature, an object which encodes the geometrical
properties coming from the Riemannian Curvature structure together with terms of perturbation due to the magnetic interaction. We will see how a positive curved Magnetic System carries a Contractible Closed Magnetic Geodesic for small energies.</span><span lang="EN-US"><o:p></o:p></span></p>
<p class="MsoNormal"><span lang="EN-US"><o:p> </o:p></span></p>
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