<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 decay of the solutions for the heat equation with a potential</dc:title>
<dc:creator>Kazuhiro Ishige</dc:creator><dc:creator>Michinori Ishiwata</dc:creator><dc:creator>Tatsuki Kawakami</dc:creator>
<dc:subject>35B40</dc:subject><dc:subject>35K15</dc:subject><dc:subject>large time behavior</dc:subject><dc:subject>heat equation</dc:subject><dc:subject>semilinear heat equation</dc:subject>
<dc:description>We study the large time behavior of the solutions for the Cauchy problem, \begin{gather*} \partial_{t} u = \Delta u + a(x,t)u \quad\mbox{in }\mathbb{R}^{N} \times (0,\infty),\\ u(x,0) = \varphi(x) \quad\mbox{in }\mathbb{R}^{N}, \end{gather*} where $\varphi \in L^{1}(\mathbb{R}^{N}, (1 + |x|^{K} )\, \mathrm{d}x)$ with $K \ge 0$ and $\| a(t) \|_{L^{\infty}(\mathbb{R}^{N})} = O(t^{-A})$ as $t \to \infty$ for some $A &gt; 1$. In this paper we classify the decay rate of the solutions and give the precise estimates on the difference between the solutions and their asymptotic profiles. Furthermore, as an application, we discuss the large time behavior of the global solutions for the semilinear heat equation, \[ \partial_{t} u= \Delta u + \lambda |u|^{p-1} u, \] where $\lambda \in \mathbb{R}$ and $p &gt; 1$.</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.2009.58.3771</dc:identifier>
<dc:source>10.1512/iumj.2009.58.3771</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 58 (2009) 2673 - 2708</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>