BMO type space associated with Neumann operator and application to a class of parabolic equations

BMO type space associated with Neumann operator and application to a class of parabolic equations
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与诺伊曼算子相关的BMO型空间及其在一类抛物方程中的应用

DOI:
10.3934/dcdsb.2021104
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发表时间:
2021
期刊:
Discrete & Continuous Dynamical Systems-B
影响因子:
--
通讯作者:
Minghua Yang
Minghua Yang
中科院分区:
其他
文献类型:
--
作者:
Zhang Chao;Minghua Yang

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Let \begin{document}$ {\rm BMO}_{\Delta_{N}}(\mathbb{R}^{n}) $\end{document} denote a BMO space on \begin{document}$ \mathbb{R}^{n} $\end{document} associated to a Neumann operator \begin{document}$ \mathcal{L}: = -\Delta_{N} $\end{document} . In this article we will show that a function \begin{document}$ f\in {\rm BMO}_{\Delta_{N}}(\mathbb{R}^{n}) $\end{document} is the trace of the solution of \begin{document}$ {\mathbb L}u = u_{t}+ \mathcal{L} u = 0, u(x, 0) = f(x), $\end{document} where \begin{document}$ u $\end{document} satisfies a Carleson-type condition \begin{document}$ \begin{eqnarray*} \sup\limits_{x_B, r_B} r_B^{-n}\int_0^{r_B^2}\int_{B(x_B, r_B)} \left\{t| \partial_t u(x, t) |^2+ | \nabla_x u(x, t) |^2 \right\}{dx dt } \leq C for some constant \begin{document}$ C>0 $\end{document} . Conversely, this Carleson condition characterizes all the \begin{document}$ {\mathbb L} $\end{document} -carolic functions whose traces belong to the space \begin{document}$ {\rm BMO}_{\Delta_{N}}(\mathbb{R}^{n}) $\end{document} . Furthermore, based on the characterization of \begin{document}$ {\rm BMO}_{\Delta_{N}}(\mathbb{R}^{n}) $\end{document} mentioned above, we prove the global well-posedness for parabolic equations of Navier-Stokes type with the Neumann boundary condition under smallness condition on the intial data \begin{document}$ u_{0}\in {{\rm BMO}_{\Delta_{N}}^{-1}(\mathbb{R}^{n})} $\end{document} .
Let \begin{document}$ {\rm BMO}_{\Delta_{N}}(\mathbb{R}^{n}) $\end{document} denote a BMO space on \begin{document}$ \mathbb{R}^{n} $\end{document} associated to a Neumann operator \begin{document}$ \mathcal{L}: = -\Delta_{N} $\end{document} . In this article we will show that a function \begin{document}$ f\in {\rm BMO}_{\Delta_{N}}(\mathbb{R}^{n}) $\end{document} is the trace of the solution of \begin{document}$ {\mathbb L}u = u_{t}+ \mathcal{L} u = 0, u(x, 0) = f(x), $\end{document} where \begin{document}$ u $\end{document} satisfies a Carleson-type condition \begin{document}$ \begin{eqnarray*} \sup\limits_{x_B, r_B} r_B^{-n}\int_0^{r_B^2}\int_{B(x_B, r_B)} \left\{t| \partial_t u(x, t) |^2+ | \nabla_x u(x, t) |^2 \right\}{dx dt } \leq C for some constant \begin{document}$ C>0 $\end{document} . Conversely, this Carleson condition characterizes all the \begin{document}$ {\mathbb L} $\end{document} -carolic functions whose traces belong to the space \begin{document}$ {\rm BMO}_{\Delta_{N}}(\mathbb{R}^{n}) $\end{document} . Furthermore, based on the characterization of \begin{document}$ {\rm BMO}_{\Delta_{N}}(\mathbb{R}^{n}) $\end{document} mentioned above, we prove the global well-posedness for parabolic equations of Navier-Stokes type with the Neumann boundary condition under smallness condition on the intial data \begin{document}$ u_{0}\in {{\rm BMO}_{\Delta_{N}}^{-1}(\mathbb{R}^{n})} $\end{document} .
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