<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>Stability of spatially periodic pulse patterns in a class of singularly perturbed reaction-diffusion equations</dc:title>
<dc:creator>Arjen Doelman</dc:creator><dc:creator>Harmen van der Ploeg</dc:creator>
<dc:subject>35B10</dc:subject><dc:subject>35B25</dc:subject><dc:subject>35B32</dc:subject><dc:subject>35B35</dc:subject><dc:subject>35K57</dc:subject><dc:subject>92C15</dc:subject><dc:subject>reaction-diffusion equations</dc:subject><dc:subject>spatially periodic solutions</dc:subject><dc:subject>stability</dc:subject><dc:subject>singular perturbations</dc:subject><dc:subject>Evans function</dc:subject>
<dc:description>In this paper we develop a stability theory for spatially periodic patterns on $\mathbb{R}$. Our approach is valid for a class of singularly perturbed reaction-diffusion equations that can be represented by the generalized Gierer-Meinhardt equations as &#39;normal form&#39;. These equations exhibit a large variety of spatially periodic patterns. We construct an Evans function $\mathcal{D}(\lambda,\gamma)$ that is defined for the $\gamma$-eigenvalue $\lambda$ in a certain subset of $\mathbb{C}$. The spectrum associated to the stability of the periodic pattern is given by the solutions $\lambda(\gamma)$ of $\mathcal{D}(\lambda(\gamma),\gamma) = 0$, where $\gamma \in \mathbf{S}^1$. Although our method can be applied to all types of singular pulse patterns, we focus on the stability analysis of the families of most simple periodic solutions. By decomposing $\mathcal{D}(\lambda,\gamma)$ into a product of a &#39;slow&#39; and a &#39;fast&#39; Evans function, we are able to determine explicit expressions for the $\gamma$-eigenvalues that are $\mathcal{O}(1)$ with respect to the small parameter $\epsilon$. Although the branch of &#39;small&#39; $\gamma$-eigenvalues that is connected to the translational $1$-eigenvalue $\lambda(1) = 0$ cannot be studied by this decomposition, our methods also enable us determine the location of these $\gamma$-eigenvalues. Thus, our approach provides a full analytical control of the (spectral) stability of the singular spatially periodic patterns. We establish that the destabilization of a periodic pulse pattern on $\mathbb{R}$ is always initiated by the $\mathcal{O}(1)$ $\gamma$-eigenvalues, and consider various kinds of bifurcations. Finally, we apply our insights to the stability problem associated to the restriction of a periodic pulse pattern to a bounded domain with homogeneous Neumann boundary conditions.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2005</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2005.54.2792</dc:identifier>
<dc:source>10.1512/iumj.2005.54.2792</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 54 (2005) 1219 - 1302</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>