Variational parabolic capacity (Q255554)
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scientific article; zbMATH DE number 6552521
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | Variational parabolic capacity |
scientific article; zbMATH DE number 6552521 |
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Variational parabolic capacity (English)
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9 March 2016
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capacity
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degenerate parabolic equations
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nonlinear potential theory
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\(p\)-parabolic equation
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The authors study a capacity related to nonlinear parabolic partial differential equations and the principal prototype is the \(p\)-parabolic equation NEWLINE\[NEWLINE \partial_t u - \mathrm{div }(| \nabla u|^{p-2}\nabla u) = 0, NEWLINE\]NEWLINE with \(p \geq 2\). The nonlinear parabolic capacity of a set \(E \subset \Omega_{\infty} = \Omega \times (0,\infty)\) is defined as NEWLINE\[NEWLINE \mathrm{cap}(E,\Omega_{\infty}) = \sup\{\mu(\Omega_{\infty}\,:\, \mathrm{supp}\,\mu \subset E,\, 0 \leq u_{\mu} \leq 1\}, NEWLINE\]NEWLINE where \(\mu\) is a non-negative Radon measure, and \(u_{\mu}\) is a weak solution to the measure data problem NEWLINE\[NEWLINE \partial_tu - \mathrm{div }(| \nabla u|^{p-2}\nabla u) = \mu, \quad \text{in } \Omega_{\infty} NEWLINE\]NEWLINE under NEWLINE\[NEWLINE u(x,t) = 0, \quad \text{for } (x, t) \in \partial_p\Omega_{\infty}. NEWLINE\]NEWLINE The nonlinear parabolic capacity has many favorable features, including inner and outer regularity. The main motivation to study such a capacity is its applications to questions regarding boundary regularity and removability. The above capacity is analogous to thermal capacity \(p = 2\) related to the heat equation. However, computing the capacities of explicit sets using the above definition is quite challenging and the aim of this paper is to develop tools for estimating capacities of explicit sets in the nonlinear parabolic context. In analogy to the elliptic situation, a central role is played by the nonlinear parabolic variational capacity which in the case of a compact set \(K\) can be written as NEWLINE\[NEWLINE \mathrm{cap}_{\mathrm{var}}(K,\Omega_{\infty}) = \{\|v\|_{W(\Omega_{\infty})}\,:\, v \in C_{0}^{\infty}(\Omega\times \mathbb{R}), v \geq \chi_{K}\} NEWLINE\]NEWLINE where \(\|v\|_{W(\Omega_{\infty})} = \|v\|^p_{\nu(\Omega_{\infty})} + \|\partial_tv\|^{p'}_{\nu(\Omega_{\infty})}\). Here \(W(\Omega_T) = \{u \in \nu(\Omega_T)\,:\, \partial_tu \in \nu(\Omega_T)\}\), \(\nu(\Omega_T) = L^p(0,W_0^{1,p}(\Omega))\) and \(\nu'(\Omega_T) = (L^p(0,W_0^{1,p}(\Omega)))'\).NEWLINENEWLINEThe main result of the paper shows that there exists a constant \(c \equiv c(n,p) > 1\) such that for any compact set \(K \subset \Omega_{\infty}\), NEWLINE\[NEWLINE c^{-1}\mathrm{cap}_{\mathrm{var}}(K,\Omega_{\infty}) \leq \mathrm{cap}(K,\Omega_{\infty}) \leq c\,\mathrm{cap}_{\mathrm{var}}(K,\Omega_{\infty}). NEWLINE\]NEWLINE As an application, the authors estimate the capacities of space-time curves, cylinders and certain hyper-surfaces.
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