Connected components of positive solutions for a Dirichlet problem involving the mean curvature operator in Minkowski space

Connected components of positive solutions for a Dirichlet problem involving the mean curvature operator in Minkowski space
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DOI:
10.3934/dcdsb.2018271
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发表时间:
2019
期刊:
Discrete & Continuous Dynamical Systems - B
影响因子:
--
通讯作者:
Ruyun Ma;Man Xu
Ruyun Ma;Man Xu
中科院分区:
其他
文献类型:
--
作者:
Ruyun Ma;Man Xu

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In this paper we study global bifurcation phenomena for the Dirichlet problem associated with the prescribed mean curvature equation in Minkowski space \begin{document}$\left\{ \begin{array}{l} -\text{div}\big(\frac{\nabla u}{\sqrt{1-|\nabla u|^2}}\big) = λ f(x,u,\nabla u)\ \ \ \ \ \ & \text{in}\ Ω,\\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ u = 0\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ & \text{on}\ \partial Ω.\\\end{array} \right.$\end{document} Here \begin{document} $Ω$ \end{document} is a bounded regular domain in \begin{document} $\mathbb{R}^N$ \end{document} , the function \begin{document} $f$ \end{document} satisfies the Caratheodory conditions, and \begin{document} $f$ \end{document} is either superlinear or sublinear in \begin{document} $u$ \end{document} at \begin{document} $0$ \end{document} . The proof of our main results are based upon bifurcation techniques.
In this paper we study global bifurcation phenomena for the Dirichlet problem associated with the prescribed mean curvature equation in Minkowski space \begin{document}$\left\{ \begin{array}{l} -\text{div}\big(\frac{\nabla u}{\sqrt{1-|\nabla u|^2}}\big) = λ f(x,u,\nabla u)\ \ \ \ \ \ & \text{in}\ Ω,\\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ u = 0\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ & \text{on}\ \partial Ω.\\\end{array} \right.$\end{document} Here \begin{document} $Ω$ \end{document} is a bounded regular domain in \begin{document} $\mathbb{R}^N$ \end{document} , the function \begin{document} $f$ \end{document} satisfies the Caratheodory conditions, and \begin{document} $f$ \end{document} is either superlinear or sublinear in \begin{document} $u$ \end{document} at \begin{document} $0$ \end{document} . The proof of our main results are based upon bifurcation techniques.