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  <title>ArcAdiA</title>
  <link rel="alternate" href="http://dspace-roma3.caspur.it:80" />
  <subtitle>The DSpace digital repository system captures, stores, indexes, preserves, and distributes digital research material.</subtitle>
  <id>http://dspace-roma3.caspur.it:80</id>
  <updated>2013-05-23T01:09:18Z</updated>
  <dc:date>2013-05-23T01:09:18Z</dc:date>
  <entry>
    <title>Asymptotic analysis for a singularly perturbed Dirichlet problem</title>
    <link rel="alternate" href="http://hdl.handle.net/2307/600" />
    <author>
      <name>Petralla, Maristella</name>
    </author>
    <id>http://hdl.handle.net/2307/600</id>
    <updated>2011-09-12T23:35:14Z</updated>
    <published>2010-05-09T22:00:00Z</published>
    <summary type="text">&lt;Title&gt;Asymptotic analysis for a singularly perturbed Dirichlet problem&lt;/Title&gt;
&lt;Authors&gt;Petralla, Maristella&lt;/Authors&gt;
&lt;Issue Date&gt;2010-05-10&lt;/Issue Date&gt;
&lt;Abstract&gt;Let us consider the problem −∆u + λV (x)u = up in Ω, u = 0 on ∂ Ω, where Ω is a smooth&#xD;
bounded domain, p &gt; 1, V is a positive potential and λ &gt; 0. We are interested in the regime λ → +∞, which is equivalent to a singularly perturbed Dirichlet problem. It is known that&#xD;
solutions u must blow up as λ → +∞, and we address here the asymptotic description of such&#xD;
a blow up behavior. When the ”energy” is uniformly bounded, the behavior is well understood&#xD;
and the solutions can develop just a ﬁnite number of sharp peaks. When V is not constant, the&#xD;
blow up points must be c.p.’s of the potential V. The situation is more involved when V = 1,&#xD;
and the crucial role is played by the mutual distances between the blow-up points as well as the&#xD;
boundary distances. The construction of these blowing-up solutions has also been addressed.&#xD;
The ﬁrst part in the thesis is devoted to strengthen such an analysis when just a Morse index&#xD;
information is available. A posteriori, we obtain an equivalence in the form of a double-side&#xD;
bound between Morse index and ”energy” with essentially optimal constants. This result can be&#xD;
seen as a sort of Rozenblyum-Lieb-Cwikel inequality, where the number of negative eigenvalues&#xD;
of a Schrodinger operator −∆ + V can be estimated in terms of a suitable Lebesgue norm of the&#xD;
negative part V− . Thanks to the speciﬁcity of our problem, we improve it by getting the correct&#xD;
Lebesgue exponent (in view of the double-side bound) as well as the sharp constants. We then&#xD;
turn to the question of concentration on manifolds of positive dimensions. The problem is well&#xD;
understood by a constructive approach but the asymptotic analysis is in general missing. Let&#xD;
us notice that on the annulus the radial ground state solution has Morse index and ”energy”&#xD;
which blow up as λ → +∞. Nonetheless, the radial Morse index is one which has allowed&#xD;
Esposito-Mancini-Santra-Srikanth to develop a ﬁne asymptotic analysis to localize the limiting&#xD;
concentration radii. They are c.p.’s of a modiﬁed potential, whose role had been already&#xD;
clariﬁed by the constructive results. The second part part of the thesis is devoted to develop an&#xD;
asymptotic analyis for solutions on the annulus which have partial symmetries. In particular,&#xD;
we consider the three-dimensional annulus and solutions which are invariant under rotations&#xD;
around the z-axis. Assuming an uniform bound on the reduced invariant Morse index, we obtain&#xD;
a localization of the limiting concentration circles in terms of a suitable modiﬁed potential. The&#xD;
main difficulty here is related to the presence of ﬁxed points w.r.t. the group action (the z-axis)&#xD;
and the aim is to exhibit potentials V for which the concentration circles (for example, for the&#xD;
ground state solution) do not degenerate to points on the z-axis.&lt;/Abstract&gt;</summary>
    <dc:date>2010-05-09T22:00:00Z</dc:date>
  </entry>
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