<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>Exponential attractors for a phase-field model with memory and quadratic nonlinearity</dc:title>
<dc:creator>Stefania Gatti</dc:creator><dc:creator>Maurizio Grasselli</dc:creator><dc:creator>Vittorino Pata</dc:creator>
<dc:subject>35B40</dc:subject><dc:subject>35B41</dc:subject><dc:subject>35Q99</dc:subject><dc:subject>37L25</dc:subject><dc:subject>37L30</dc:subject><dc:subject>45K05</dc:subject><dc:subject>80A22</dc:subject><dc:subject>phase-field models</dc:subject><dc:subject>memory effects</dc:subject><dc:subject>infinite-dimensional dissipative dynamical systems</dc:subject><dc:subject>invariant absorbing sets</dc:subject><dc:subject>universal attractor</dc:subject><dc:subject>exponential attractors</dc:subject><dc:subject>fractal dimension</dc:subject>
<dc:description>We consider a phase-field system with memory effects. This model consists of an integrodifferential equation of parabolic type describing the evolution of the (relative) temperature $\theta$, and depending on its past history. This equation is nonlinearly coupled through a function $\lambda$ with a semilinear parabolic equation governing the order parameter $\chi$. The state variables $\theta$ and $\chi$ are subject to Neumann homogeneous boundary conditions. The model becomes an infinite-dimensional dynamical system in a suitable phase-space by introducing an additional variable $\eta$ accounting for the (integrated) past history of the temperature. The evolution of $\eta$ is thus ruled by a first-order hyperbolic equation. Giorgi, Grasselli, and Pata proved that the obtained dynamical system possesses a universal attractor $\mathcal{A}$, which has finite fractal dimension provided that the coupling function $\lambda$ is linear. Here we prove, as main result, the existence of an exponential attractor $\mathcal{E}$ which entails, in particular, that $\mathcal{A}$ has finite fractal dimension when $\lambda$ is nonlinear with quadratic growth. Since the so-called squeezing property does not work in our framework, we cannot use the standard technique to construct $\mathcal{E}$. Instead, we take advantage of a recent result due to Efendiev, Miranville, and Zelik. The present paper contains, to the best of our knowledge, the first example of exponential attractor for an infinite-dimensional dynamical system with memory effects. Also, the approach introduced here can be adapted to other dynamical systems with similar features.</dc:description>
<dc:publisher>Indiana University Mathematics Journal</dc:publisher>
<dc:date>2004</dc:date>
<dc:type>text</dc:type>
<dc:format>pdf</dc:format>
<dc:identifier>10.1512/iumj.2004.53.2413</dc:identifier>
<dc:source>10.1512/iumj.2004.53.2413</dc:source>
<dc:language>en</dc:language>
<dc:relation>Indiana Univ. Math. J. 53 (2004) 719 - 754</dc:relation>
<dc:coverage>state-of-the-art mathematics</dc:coverage>
<dc:rights>http://iumj.org/access/</dc:rights>
</oai_dc:dc>