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   	<dc:title>Viscoelastic Cahn–Hilliard models for tumor growth</dc:title>
   	<dc:creator>Garcke, Harald</dc:creator>
   	<dc:creator>Kovács, Balázs</dc:creator>
   	<dc:creator>Trautwein, Dennis</dc:creator>
   	<dc:subject>Applied Mathematics</dc:subject>
   	<dc:subject>Modeling and Simulation</dc:subject>
   	<dc:description>&lt;jats:p&gt; We introduce a new phase field model for tumor growth where viscoelastic effects are taken into account. The model is derived from basic thermodynamical principles and consists of a convected Cahn–Hilliard equation with source terms for the tumor cells and a convected reaction–diffusion equation with boundary supply for the nutrient. Chemotactic terms, which are essential for the invasive behavior of tumors, are taken into account. The model is completed by a viscoelastic system consisting of the Navier–Stokes equation for the hydrodynamic quantities, and a general constitutive equation with stress relaxation for the left Cauchy–Green tensor associated with the elastic part of the total mechanical response of the viscoelastic material. For a specific choice of the elastic energy density and with an additional dissipative term accounting for stress diffusion, we prove existence of global-in-time weak solutions of the viscoelastic model for tumor growth in two space dimensions [Formula: see text] by the passage to the limit in a fully-discrete finite element scheme where a CFL condition, i.e. [Formula: see text], is required. &lt;/jats:p&gt;&lt;jats:p&gt; Moreover, in arbitrary dimensions [Formula: see text], we show stability and existence of solutions for the fully-discrete finite element scheme, where positive definiteness of the discrete Cauchy–Green tensor is proved with a regularization technique that was first introduced by Barrett and Boyaval [Existence and approximation of a (regularized) Oldroyd-B model, Math. Models Methods Appl. Sci. 21 (2011) 1783–1837]. After that, we improve the regularity results in arbitrary dimensions [Formula: see text] and in two dimensions [Formula: see text], where a CFL condition is required. Then, in two dimensions [Formula: see text], we pass to the limit in the discretization parameters and show that subsequences of discrete solutions converge to a global-in-time weak solution. Finally, we present numerical results in two dimensions [Formula: see text]. &lt;/jats:p&gt;</dc:description>
   	<dc:publisher>World Scientific Pub Co Pte Ltd</dc:publisher>
   	<dc:date>2022</dc:date>
   	<dc:type>info:eu-repo/semantics/article</dc:type>
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   	<dc:type>text</dc:type>
   	<dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
   	<dc:identifier>https://ris.uni-paderborn.de/record/45970</dc:identifier>
   	<dc:source>Garcke H, Kovács B, Trautwein D. Viscoelastic Cahn–Hilliard models for tumor growth. &lt;i&gt;Mathematical Models and Methods in Applied Sciences&lt;/i&gt;. 2022;32(13):2673-2758. doi:&lt;a href=&quot;https://doi.org/10.1142/s0218202522500634&quot;&gt;10.1142/s0218202522500634&lt;/a&gt;</dc:source>
   	<dc:language>eng</dc:language>
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   	<dc:relation>info:eu-repo/semantics/altIdentifier/issn/0218-2025</dc:relation>
   	<dc:relation>info:eu-repo/semantics/altIdentifier/issn/1793-6314</dc:relation>
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