<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>Existence of a solution to a vector-valued Allen-Cahn equation with a three well potential</dc:title>
<dc:creator>Mariel Saez Trumper</dc:creator>
<dc:subject>35J15</dc:subject><dc:subject>35J60</dc:subject><dc:subject>35J65</dc:subject><dc:subject>vector-valued Allen-Cahn-equation</dc:subject><dc:subject>3 well potential</dc:subject><dc:subject>multiple well potential</dc:subject><dc:subject>phase transition</dc:subject><dc:subject>triple junction</dc:subject>
<dc:description>In this paper we prove the existence of a vector-valued solution $v$ to \begin{gather*} -\Delta v + \frac{\nabla_vW(v)}{2} = 0, \\\lim_{r\to\infty}v(r\cos\theta,r\sin\theta) = c_i\quad\mbox {for} \theta\in(\theta_{i-1},\theta_i),\end{gather*} where $W:\mathbb{R}^2\to\mathbb{R}$ is a non-negative function that attains its minimum $0$ at $\{c_i\}_{i=1}^3$, and the angles $\theta_i$ are determined by the function $W$. This solution is an energy minimizer.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2009</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2009.58.3233</dc:identifier>
<dc:source>10.1512/iumj.2009.58.3233</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 58 (2009) 213 - 268</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>