<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>Segregated vector solutions for linearly coupled nonlinear Schrodinger systems</dc:title>
<dc:creator>Chang-Shou Lin</dc:creator><dc:creator>Shuangjie Peng</dc:creator>
<dc:subject>35J60</dc:subject><dc:subject>segregation</dc:subject><dc:subject>concentration</dc:subject><dc:subject>multi-bump solutions</dc:subject><dc:subject>phase seperations</dc:subject><dc:subject>Nonlinear Schrodinger equation</dc:subject>
<dc:description>We consider the system linearly coupled by nonlinear
Schr\&quot;odinger equations in $\R^3$:
\[
\left\{
\begin{array}{ll}
-\Delta u_j+u_j=u^3_j-\va\sum\limits_{i\neq j}^N u_i,\hspace{2mm} x\in \R^3, \vspace{0.2cm}\\
u_j\in H^1(\R^3),\quad j=1,\cdots,N,
\end{array}
\right.
\]
where $\va\in\R$ is a coupling constant. This type of system arises in particular in models in nonlinear $N$-core fiber.

We then examine how the linear coupling affects the solution structure. When $N=2,3$, for any prescribed integer $\ell\ge 2$, we
construct a nonradial vector solution of segregated type, with two components having exactly $\ell$ positive bumps for $\va&gt;0$ sufficiently small. We also give an explicit description of the characteristic features of the vector solutions.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2014</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2014.63.5310</dc:identifier>
<dc:source>10.1512/iumj.2014.63.5310</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 63 (2014) 939 - 967</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>