<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>Asymptotic behavior for a viscous Hamilton-Jacobi equation with critical exponent</dc:title>
<dc:creator>Thierry Gallay</dc:creator><dc:creator>Philippe Laurencot</dc:creator>
<dc:subject>35B33</dc:subject><dc:subject>35B40</dc:subject><dc:subject>35K55</dc:subject><dc:subject>37L25</dc:subject><dc:subject>diffusive Hamilton-Jacobi equation</dc:subject><dc:subject>large time behavior</dc:subject><dc:subject>critical exponent</dc:subject><dc:subject>absorption</dc:subject><dc:subject>invariant manifold</dc:subject><dc:subject>self-similarity</dc:subject>
<dc:description>The large time behavior of non-negative solutions to the viscous Hamilton-Jacobi equation $\partial_t u - \Delta u + |\nabla  u|^q = 0$ in $(0,\infty) \times \mathbb{R}^N$ is investigated for the critical exponent $q = (N+2)/(N+1)$. Convergence towards a rescaled self-similar solution to the linear heat equation is shown, the rescaling factor being $(\ln{t})^{-(N+1)}$. The proof relies on the construction of a one-dimensional invariant manifold for a suitable truncation of the equation written in self-similar variables.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2007</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2007.56.3107</dc:identifier>
<dc:source>10.1512/iumj.2007.56.3107</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 56 (2007) 459 - 480</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>