<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 relationship between two-parameter perturbed sine-Gorden type equation and nonlinear Klein-Gordon equation</dc:title>
<dc:creator>Tetsutaro Shibata</dc:creator>
<dc:subject>34B15</dc:subject><dc:subject>two-parameter</dc:subject><dc:subject>perturbed sine-Gordon</dc:subject>
<dc:description>We consider the two-parameter nonlinear eigenvalue problem of perturbed sine-Gordon type: \begin{multline*} u&#39;&#39;(t) + \mu u(t) = \lambda g(u(t)),\\ u(t) &gt; 0 \mbox{ in } I := (0,1), \quad u(0) = u(1) = 0, \end{multline*} where $\mu$, $\lambda &gt; 0$ are parameters and $g(u) = a_{1}u - a_{2}u^{p} + o(u^{p})$ as $u \downarrow 0$ ($p \ge 3$, $a_{1}$, $a_{2} &gt; 0$). This equation is called a perturbed sine-Gordon type equation when $g(u) = u + \sin u$. By using a variational method on general level sets, we establish the different types of asymptotic formulas for the solutions as $\mu \to \infty$ for the case $p &gt; 5$, $p = 5$, $3 &lt; p &lt; 5$, and $p = 3$, respectively. We emphasize that critical exponents are $p = 3$, $5$ and only in the case where $p = 3$, the solution of the above equation is related asymptotically to that of the associated nonlinear stationary Klein-Gordon equation as $\mu \to \infty$.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2006</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2006.55.2812</dc:identifier>
<dc:source>10.1512/iumj.2006.55.2812</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 55 (2006) 1557 - 1572</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>