<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>On compound vortices in a two-component Ginzburg-Landau functional</dc:title>
<dc:creator>Stanley Alama</dc:creator><dc:creator>Lia Bronsard</dc:creator><dc:creator>Petru Mironescu</dc:creator>
<dc:subject>35J50</dc:subject><dc:subject>35J57</dc:subject><dc:subject>35Q56</dc:subject><dc:subject>Partial Differential Equations</dc:subject><dc:subject>Calculus of Variations</dc:subject><dc:subject>Bifurcations</dc:subject>
<dc:description>We study the structure of vortex solutions in a Ginzburg-Landau system for two complex-valued order parameters. We consider the Dirichlet problem in the disk in $mathbb{R}^2$ with symmetric, degree-one boundary condition, as well as the associated degree-one entire solutions in all of $mathbb{R}^2$. Each problem has degree-one equivariant solutions with radially symmetric profile vanishing at the origin, of the same form as the unique (complex scalar) Ginzburg-Landau minimizer. We find that there is a range of parameters for which these equivariant solutions are the unique locally energy-minimizing solutions for the coupled system. Surprisingly, there is also a parameter regime in which the equivariant solutions are unstable, and minimizers must vanish separately in each component of the order parameter.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2012</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2012.61.4737</dc:identifier>
<dc:source>10.1512/iumj.2012.61.4737</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 61 (2012) 1861 - 1909</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>