L¹条件下含分段积分的BV空间定义泛函的逼近

Thomas Wunderli
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引用次数: 0

摘要

我们证明了一类泛函$% %TCIMACRO{\TeXButton{mathcal G}{\mathcal{G}} % %BeginExpansion \mathcal{G}% % endexpand (u)=\int_{\Omega}\varphi (x,Du)$定义在$BV\left(\Omega \right) $上,其中$\varphi (\cdot,Du)\in L^{1}\left(\Omega \right) $,$ $\Omega \子集%TCIMACRO{\ u {211d}}% BeginExpansion \mathbb{R} % endexpand ^{N}$有界,$ \varphi (x,p)$凸,径向对称的形式为\begin{equation*} \varphi (x,p)=\left\{\begin{tabular}{ll} $g(x,p)$ &如果$|p|\leq \beta $\ \ $\psi (x)|p|+k(x)$ &如果$|p|>\beta .$% \end{tabular}% \right。我们显示每个$u\在BV\左(\Omega \右)\ cap L^{p}\左(\Omega \右),$ $1\leq p<\infty,$ $存在$u_{k}\在W^{1,1}\左(\Omega \右)\ cap C^{\infty}\左(\Omega \右)\ cap L^{p}\左(\Omega \右)$因此$% %TCIMACRO{\TeXButton{mathcal G}{\mathcal{G}} % %BeginExpansion \mathcal{G}} % %BeginExpansion \mathcal{G}} % %BeginExpansion \mathcal{G}} % % endexpand (u_{k})\right row %TCIMACRO{\TeXButton{mathcal G}} {\mathcal{G}} % %BeginExpansion \mathcal{G}% % endexpand (u).$ BV$中的近似定理被使用证明时间流$u_{t}=\func{div}\left(\nabla _{p}\varphi (x,Du\right))$ in $L^{1}((0,\infty))$的强解的存在性结果;BV\left(\Omega \right) \cap L^{p}\left(\Omega \right))$通常在$u$中附加边界条件或惩罚项以确保唯一性。本工作中的函数没有被先前的近似定理所涵盖,因为对于固定的$p$,我们有$\varphi (x,p)\in L^{1}\left(\Omega \right) $,这在早期的工作中通常不适用于$\varphi $的假设。
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Approximation of BV space-defined Functionals Containing Piecewise Integrands with L¹ Condition
We prove an approximation result for a class of functionals $% %TCIMACRO{\TeXButton{mathcal G}{\mathcal{G}}}% %BeginExpansion \mathcal{G}% %EndExpansion (u)=\int_{\Omega }\varphi (x,Du)$ defined on $BV\left( \Omega \right) $ where $\varphi (\cdot ,Du)\in L^{1}\left( \Omega \right) ,$ $\Omega \subset %TCIMACRO{\U{211d} }% %BeginExpansion \mathbb{R} %EndExpansion ^{N}$ bounded, $\varphi (x,p)$ convex, radially symmetric and of the form \begin{equation*} \varphi (x,p)=\left\{ \begin{tabular}{ll} $g(x,p)$ & if $|p|\leq \beta $ \\ $\psi (x)|p|+k(x)$ & if $|p|>\beta .$% \end{tabular}% \right. \end{equation*}% We show for each $u\in BV\left( \Omega \right) \cap L^{p}\left( \Omega \right) ,$ $1\leq p<\infty ,$ there exist $u_{k}\in W^{1,1}\left( \Omega \right) \cap C^{\infty }\left( \Omega \right) \cap L^{p}\left( \Omega \right) $ so that $% %TCIMACRO{\TeXButton{mathcal G}{\mathcal{G}}}% %BeginExpansion \mathcal{G}% %EndExpansion (u_{k})\rightarrow %TCIMACRO{\TeXButton{mathcal G}{\mathcal{G}}}% %BeginExpansion \mathcal{G}% %EndExpansion (u).$ Approximation theorems in $BV$ are used to prove existence results for the strong solution to the time flow $u_{t}=\func{div}\left( \nabla _{p}\varphi (x,Du\right) )$ in $L^{1}((0,\infty );BV\left( \Omega \right) \cap L^{p}\left( \Omega \right) ),$ typically with additional boundary condition or penalty term in $u$ to ensure uniqueness. The functions in this work are not covered by previous approximation theorems since for fixed $p$ we have $\varphi (x,p)\in L^{1}\left( \Omega \right) $ which do not in general hold for assumptions on $\varphi $ in earlier work.
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