<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>The Keller-Segel system of parabolic-parabolic type with initial data in weak  $L^{n/2}(\mathbb{R}^n)$ and its application to self-similar solutions</dc:title>
<dc:creator>Hideo Kozono</dc:creator><dc:creator>Yoshie Sugiyama</dc:creator>
<dc:subject>35Q30</dc:subject><dc:subject>Keller-Segel system</dc:subject><dc:subject>self-similar solution</dc:subject><dc:subject>BMO space</dc:subject><dc:subject>weak $L^p$-space</dc:subject><dc:subject>heat semigroup</dc:subject>
<dc:description>We shall show the existence of a \emph{global} strong solution to the semilinear Keller-Segel system in $\mathbb{R}^{n}$, $n \ge 3$ of \emph{parabolic-parabolic type} with small initial data $u_{0} \in L_{w}^{n/2}(\mathbb{R}^{n})$ and $v_{0} \in \mathrm{BMO}$. Our method is based on the perturbation of linearization together with the $L^{p} - L^{q}$-estimates of the heat semigroup and the fractional powers of the Laplace operator. As a by-product of our method, we shall construct a self-similar solution and prove the smoothing effect. Furthermore, the stability problem on our strong solutions will be also discussed.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2008</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2008.57.3316</dc:identifier>
<dc:source>10.1512/iumj.2008.57.3316</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 57 (2008) 1467 - 1500</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>