<oai_dc: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>Stability in $2D$ Ginzburg-Landau passes to the limit</dc:title>
<dc:creator>Sylvia Serfaty</dc:creator>
<dc:subject>35B38</dc:subject><dc:subject>35B40</dc:subject><dc:subject>35B35</dc:subject><dc:subject>35B25</dc:subject><dc:subject>35Q99</dc:subject><dc:subject>Ginzburg-Landau</dc:subject><dc:subject>vortices</dc:subject><dc:subject>stability</dc:subject><dc:subject>asymptotics</dc:subject>
<dc:description>We prove that if we consider a family of \textit{stable} solutions to the Ginzburg-Landau equation, then their vortices converge to a \textit{stable} critical point of the ``renormalized energy.&#39;&#39; Moreover, in the case of instability, the number of ``directions of descent&#39;&#39; is bounded below by the number of directions of descent for the renormalized energy. A consequence is a result of nonexistence of stable nonconstant solutions to Ginzburg-Landau with homogeneous Neumann boundary condition.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2005</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2005.54.2497</dc:identifier>
<dc:source>10.1512/iumj.2005.54.2497</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 54 (2005) 199 - 222</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>