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Wenming Zou

Publications and source records attributed to Wenming Zou.

At least 73 records · Page 4Linked to original sources

On a double-variable inequality and elliptic systems involving critical Hardy-Sobolev exponents

Let $Ω\subset \mathbb{R}^N$ ($N\geq 3$) be an open domain which is not necessarily bounded. The sharp constant and extremal functions to the following kind of double-variable inequalities $$ S_{α,β,λ,μ}(Ω) \Big(\int_Ω\big(λ\frac{|u|^{2^*(s)}}{|x|^s}+μ\frac{|v|^{2^*(s)}}{|x|^s}+2^*(s)κ\frac{|u|^α|v|^β}{|x|^s}\big)dx\Big)^{\frac{2}{2^*(s)}}$$ $$\leq \int_Ω\big(|\nabla u|^2+|\nabla v|^2\big)dx$$ for $(u,v)\in {\mathscr{D}}:=D_{0}^{1,2}(Ω)\times D_{0}^{1,2}(Ω)$ will be explored. Further results about the sharp constant $S_{α,β,λ,μ}(Ω)$ with its extremal functions when $Ω$ is a general open domain will be involved. For this goal, we consider the following elliptic systems involving multiple Hardy-Sobolev critical exponents: $$\begin{cases} -Δu-λ\frac{|u|^{2^*(s_1)-2}u}{|x|^{s_1}}=κα\frac{1}{|x|^{s_2}}|u|^{α-2}u|v|^β\quad &\hbox{in}\;Ω, -Δv-μ\frac{|v|^{2^*(s_1)-2}v}{|x|^{s_1}}=κβ\frac{1}{|x|^{s_2}}|u|^α|v|^{β-2}v\quad &\hbox{in}\;Ω, (u,v)\in \mathscr{D}:=D_{0}^{1,2}(Ω)\times D_{0}^{1,2}(Ω), \end{cases}$$ where $s_1,s_2\in (0,2), α>1,β>1, λ>0,μ>0,κ\neq 0, α+β\leq 2^*(s_2)$. Here, $2^*(s):=\frac{2(N-s)}{N-2}$ is the critical Hardy-Sobolev exponent. We mainly study the critical case (i.e., $α+β=2^*(s_2)$) when $Ω$ is a cone (in particular, $Ω=\mathbb{R}_+^N$ or $Ω=\mathbb{R}^N$). We will establish a sequence of fundamental results including regularity, symmetry, existence and multiplicity, uniqueness and nonexistence, {\it etc.}

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$p$-Laplacian problems involving critical Hardy-Sobolev exponents

We prove existence, multiplicity, and bifurcation results for $p$-Laplacian problems involving critical Hardy-Sobolev exponents. Our results are mainly for the case $λ\ge λ_1$ and extend results in the literature for $0 < λ< λ_1$. In the absence of a direct sum decomposition, we use critical point theorems based on a cohomological index and a related pseudo-index.

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On finite Morse index solutions to the quadharmonic Lane-Emden equation

In this paper, we compute the Joseph-Lundgren exponent for the quadharmonic Lane-Emden equation, derive a monotonicity formula and classify the finite Morse index solution to the following quadharmonic Lane-Emden equation: \noindent \begin{equation}\nonumber Δ^4 u=|u|^{p-1}u\;\;\;\;\hbox{in}\;\;\;\;\; \R^n. \end{equation} As a byproduct, we also get a monotonicity formula for the quadharmonic maps $ Δ^4 u=0$.

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Existence, nonexistence, symmetry and uniqueness of ground state for critical Schrödinger system involving Hardy term

We study the following elliptic system with critical exponent: \begin{displaymath} \begin{cases}-Δu_j-\frac{λ_j}{|x|^2}u_j=u_j^{2^*-1}+\sum\limits_{k\neq j}β_{jk}α_{jk}u_j^{α_{jk}-1}u_k^{α_{kj}},\;\;x\in\R^N, u_j\in D^{1,2}(\R^N),\quad u_j>0 \;\; \hbox{in} \quad \R^N\setminus \{0\},\quad j=1,...,r.\end{cases}\end{displaymath} Here $N\geq 3, r\geq2, 2^*=\frac{2N}{N-2}, λ_j\in (0, \frac{(N-2)^2}{4})$ for all $ j=1,...,r $; $β_{jk}=β_{kj}$; \; $α_{jk}>1, α_{kj}>1,$ satisfying $α_{jk}+α_{kj}=2^* $ for all $k\neq j$. Note that the nonlinearities $u_j^{2^*-1}$ and the coupling terms all are critical in arbitrary dimension $N\geq3 $. The signs of the coupling constants $\bb_{ij}$'s are decisive for the existence of the ground state solutions. We show that the critical system with $r\geq 3$ has a positive least energy solution for all $β_{jk}>0$. However, there is no ground state solutions if all $β_{jk}$ are negative. We also prove that the positive solutions of the system are radially symmetric. Furthermore, we obtain the uniqueness theorem for the case $r\geq 3$ with $N=4$ and the existence theorem when $r=2$ with general coupling exponents.

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On the triharmonic Lane-Emden equation

We derive a monotonicity formula and classify finite Morse index solutions (positive or sign-changing, radial or not) to the following triharmonic Lane-Emden equation: \begin{equation}\nonumber (-Δ)^3 u=|u|^{p-1}u \hbox{ in } \mathbb{R}^n, \end{equation} where $p$ is below the Joseph-Lundgren exponent. As a byproduct we also obtain a new monotonicity formula for the triharmonic maps.

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Multiplicity and concentration behavior of solutions to the critical Kirchhoff type problem

In this paper, we study the multiplicity and concentration of the positive solutions to the following critical Kirchhoff type problem: \begin{equation*} -\left(\varepsilon^2 a+\varepsilon b\int_{\R^3}|\nabla u|^2\mathrm{d} x\right)Δu + V(x) u = f(u)+u^5\ \ {\rm in } \ \ \R^3, \end{equation*} where $\varepsilon$ is a small positive parameter, $a$, $b$ are positive constants, $V \in C(\mathbb{R}^3)$ is a positive potential, $f \in C^1(\R^+, \R)$ is a subcritical nonlinear term, $u^5$ is a pure critical nonlinearity. When $\varepsilon>0$ small, we establish the relationship between the number of positive solutions and the profile of the potential $V$. The exponential decay at infinity of the solution is also obtained. In particular, we show that each solution concentrates around a local strict minima of $V$ as $\varepsilon \rightarrow 0$.

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On the equation $p \frac{Γ(\frac{n}{2}-\frac{s}{p-1})Γ(s+\frac{s}{p-1})}{Γ(\frac{s}{p-1})Γ(\frac{n-2s}{2}-\frac{s}{p-1})} =\frac{Γ(\frac{n+2s}{4})^2}{Γ(\frac{n-2s}{4})^2}$

The note is aimed at giving a complete characterization of the following equation: $$\displaystyle p\frac{Γ(\frac{n}{2}-\frac{s}{p-1})Γ(s+\frac{s}{p-1})}{Γ(\frac{s}{p-1})Γ(\frac{n-2s}{2}-\frac{s}{p-1})} =\frac{Γ(\frac{n+2s}{4})^2}{Γ(\frac{n-2s}{4})^2}.$$ The method is based on some key transformation and the properties of the Gamma function. Applications to fractional nonlinear Lane-Emden equations will be given.

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The Nehari manifold for fractional systems involving critical nonlinearities

We study the combined effect of concave and convex nonlinearities on the number of positive solutions for a fractional system involving critical Sobolev exponents. With the help of the Nehari manifold, we prove that the system admits at least two positive solutions when the pair of parameters $(λ,μ)$ belongs to a suitable subset of $\R^2$.

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On critical $p$-Laplacian systems

We consider the critical $p$-Laplacian system \begin{equation}\label{92} \begin{cases}-Δ_p u-\frac{λa}{p}|u|^{a-2}u|v|^b =μ_1|u|^{p^\ast-2}u+\frac{αγ}{p^\ast}|u|^{α-2}u|v|^β, &x\inΩ,\\ -Δ_p v-\frac{λb}{p}|u|^a|v|^{b-2}v =μ_2|v|^{p^\ast-2}v+\frac{βγ}{p^\ast}|u|^α|v|^{β-2}v, &x\inΩ,\\ u,v\ \text{in } D_0^{1,p}(Ω), \end{cases} \end{equation} where $Δ_p:=\text{div}(|\nabla u|^{p-2}\nabla u)$ is the $p$-Laplacian operator defined on $D^{1,p}(\mathbb{R}^N):=\{u\in L^{p^\ast}(\mathbb{R}^N):|\nabla u|\in L^p(\mathbb{R}^N)\}$, endowed with norm $\|u\|_{D^{1,p}}:=\big(\int_{\mathbb{R}^N}|\nabla u|^p\text{d}x\big)^{\frac{1}{p}}$, $N\ge3$, $1 1$ satisfy $a + b = p, α+ β= p^\ast:=\frac{Np}{N-p}$, the critical Sobolev exponent, $Ω$ is $\mathbb{R}^N$ or a bounded domain in $\mathbb{R}^N$, $D_0^{1,p}(Ω)$ is the closure of $C_0^\infty(Ω)$ in $D^{1,p}(\mathbb{R}^N)$. Under suitable assumptions, we establish the existence and nonexistence of a positive least energy solution. We also consider the existence and multiplicity of nontrivial nonnegative solutions.

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On Elliptic Systems involving critical Hardy-Sobolev exponents

Let $Ω\subset \R^N$ ($N\geq 3$) be an open domain which is not necessarily bounded. By using variational methods, we consider the following elliptic systems involving multiple Hardy-Sobolev critical exponents: $$\begin{cases} -Δu-λ\frac{|u|^{2^*(s_1)-2}u}{|x|^{s_1}}=κα\frac{1}{|x|^{s_2}}|u|^{α-2}u|v|^β\quad &\hbox{in}\;Ω,\\ -Δv-μ\frac{|v|^{2^*(s_1)-2}v}{|x|^{s_1}}=κβ\frac{1}{|x|^{s_2}}|u|^α|v|^{β-2}v\quad &\hbox{in}\;Ω,\\ (u,v)\in \mathscr{D}:=D_{0}^{1,2}(Ω)\times D_{0}^{1,2}(Ω), \end{cases}$$ where $s_1,s_2\in (0,2), α>1,β>1, λ>0,μ>0,κ\neq 0, α+β\leq 2^*(s_2)$. Here, $2^*(s):=\frac{2(N-s)}{N-2}$ is the critical Hardy-Sobolev exponent. We mainly study the critical case (i.e., $α+β=2^*(s_2)$) when $Ω$ is a cone (in particular, $Ω=\R_+^N$ or $Ω=\R^N$). We will establish a sequence of fundamental results including regularity, symmetry, existence and multiplicity, uniqueness and nonexistence, {\it etc.} In particular, the sharp constant and extremal functions to the following kind of double-variable inequalities $$ S_{α,β,λ,μ}(Ω) \Big(\int_Ω\big(λ\frac{|u|^{2^*(s)}}{|x|^s}+μ\frac{|v|^{2^*(s)}}{|x|^s}+2^*(s)κ\frac{|u|^α|v|^β}{|x|^s}\big)dx\Big)^{\frac{2}{2^*(s)}}$$ $$\leq \int_Ω\big(|\nabla u|^2+|\nabla v|^2\big)dx$$ for $(u,v)\in {\mathscr{D}} $ will be explored. Further results about the sharp constant $S_{α,β,λ,μ}(Ω)$ with its extremal functions when $Ω$ is a general open domain will be involved.

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On Elliptic Systems involving critical Hardy-Sobolev exponents (Part II)

This paper is the second part of a work devoted to the study of elliptic systems involving multiple Hardy-Sobolev critical exponents: $$\begin{cases} -Δu-λ\frac{|u|^{2^*(s_1)-2}u}{|x|^{s_1}}=κα\frac{1}{|x|^{s_2}}|u|^{α-2}u|v|^β\quad &\hbox{in}\;Ω,\\ -Δv-μ\frac{|v|^{2^*(s_1)-2}v}{|x|^{s_1}}=κβ\frac{1}{|x|^{s_2}}|u|^α|v|^{β-2}v\quad &\hbox{in}\;Ω,\\ κ>0,(u,v)\in \mathscr{D}:=D_{0}^{1,2}(Ω)\times D_{0}^{1,2}(Ω), \end{cases}$$ where $s_1\neq s_2\in (0,2), α>1,β>1, λ>0,μ>0,κ>0, α+β=2^*(s_2)$. Here, $2^*(s):=\frac{2(N-s)}{N-2}$ is the critical Hardy-Sobolev exponent. When $Ω$ is a cone (especially $Ω=\R_+^N$ or $Ω=\R^N$), we study the existence of positive ground state solution.

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A perturbed nonlinear elliptic PDE with two Hardy-Sobolev critical exponents

Let $Ω$ be a $C^1$ open bounded domain in $\R^N$ ($N\geq 3$) with $0\in \partial Ω$. Suppose that $\partialΩ$ is $C^2$ at $0$ and the mean curvature of $\partialΩ$ at $0$ is negative. Consider the following perturbed PDE involving two Hardy-Sobolev critical exponents: $$ \begin{cases} &Δu+λ_1 \frac{u^{2^*(s_1)-1}}{|x|^{s_1}}+λ_2\frac{u^{2^*(s_2)-1}}{|x|^{s_2}}+λ_3\frac{u^p}{|x|^{s_3}}=0\;\quad \hbox{in}\;Ω,\\ &u(x)>0\;\hbox{in}\;Ω,\;\, u(x)=0\;\hbox{on}\;\partialΩ, \end{cases} $$ where $0 0, 1< p\leq 2^*(s_3)-1$. The existence of ground state solution is studied under different assumptions via the concentration compactness principle and the Nehari manifold method. We also apply a perturbation method to study the existence of positive solution.

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On a doubly critical Schrödinger system in $\bbr^4$ with steep potential wells

Study the following two-component elliptic system% \begin{equation*} \left\{\aligned&Δu-(λa(x)+a_0)u+u^3+βv^2u=0\quad&\text{in }\bbr^4,\\% &Δv-(λb(x)+b_0)v+v^3+βu^2v=0\quad&\text{in }\bbr^4,\\% &(u,v)\in\h\times\h,\endaligned\right.% \end{equation*} where $a_0,b_0\in\bbr$ are constants; $λ>0$ and $β\in\bbr$ are parameters and $a(x), b(x)\geq0$ are potential wells which are not necessarily to be radial symmetric. By using the variational method, we investigate the existence of ground state solutions and general ground state solutions (i.e., possibly semi-trivial) to this system. Indeed, to the best of our knowledge, even the existence of semi-trivial solutions is also unknown in the literature. We observe some concentration behaviors of ground state solutions and general ground state solutions. The phenomenon of phase separations is also excepted. It seems that this is the first result definitely describing the phenomenon of phase separation for critical system in the whole space $\bbr^4$. Note that both the cubic nonlinearities and the coupled terms of the system are all of critical growth with respect to the Sobolev critical exponent.

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Existence of extremal functions for a family of Caffarelli-Kohn-Nirenberg inequalities

Consider the following inequalities due to Caffarelli, Kohn and Nirenberg {\it (Compositio Mathematica,1984):} $$\Big(\int_Ω\frac{|u|^r}{|x|^s}dx\Big)^{\frac{1}{r}}\leq C(p,q,r,μ,σ,s)\Big(\int_Ω\frac{|\nabla u|^p}{|x|^μ}dx\Big)^{\frac{a}{p}}\Big(\int_Ω\frac{|u|^q}{|x|^σ}dx\Big)^{\frac{1-a}{q}},$$ where $Ω\subset \R^N (N\geq 2)$ is an open set; $p, q, r, μ, σ, s, a$ are some parameters satisfying some balanced conditions. When $Ω$ is a cone in $\R^N$ (for example, $Ω=\R^N)$, we prove the sharp constant $C(p,q,r,μ,σ,s)$ can be achieved for a very large parameter space. Besides, we find some sufficient conditions which guarantee that the following Sobolev spaces $$W_μ^{1,p}(Ω),\; W_μ^{1,p}(Ω)\cap L^p(Ω), \; H^{1,p}(\R^N) $$ are compactly embedded into $L^r(\R^N, \frac{dx}{|x|^s})$ for some new ranges of parameters, where $\displaystyle W_μ^{1,p}(Ω)$ is the completion of $C_0^\infty(Ω)$ with respect to the norm $\displaystyle \Big(\int_Ω\frac{ |\nabla u|^p}{|x|^μ}dx\Big)^{\frac{1}{p}}. $ As applications, we also study the equation $$\displaystyle -div\Big(\frac{|\nabla u|^{p-2}\nabla u}{|x|^μ}\Big)=λV(x)|u|^{q-2}u, \;\;\; u\in W_μ^{1,p}(Ω)$$ under some proper conditions on $V(x)$.

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On coupled Schrödinger systems with double critical exponents and indefinite weights

By using variational methods, we study the existence of mountain pass solution to the following doubly critical Schrödinger system: $$ \begin{cases} -Δu-μ_1\frac{u}{|x|^2}-|u|^{2^{*}-2}u &=h(x)α|u|^{α-2}|v|^βu\quad \rm{in}\; \R^N, -Δv-μ_2\frac{v}{|x|^2}-|v|^{2^{*}-2}v &= h(x)β|u|^α|v|^{β-2}v\quad \rm{in}\; \R^N, \end{cases} $$ where $α\geq 2, β\geq 2, α+β\leq 2^*$;\; $ μ_1, μ_2\in [0, \frac{(N-2)^2}{4})$. The weight function $h(x)$ is allowed to be sign-changing so that the nonlinearities include a large class of indefinite weights. We show that the $PS$ condition is satisfied at higher energy level when $α+β=2^*$ and obtain the existence of mountain pass solution. Besides, a nonexistence result of the ground state is given.

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On a two-component Bose-Einstein condensate with steep potential wells

In this paper, we study the following two-component systems of nonlinear Schrödinger equations \begin{equation*} \left\{\aligned&Δu-(λa(x)+a_0(x))u+μ_1u^3+βv^2u=0\quad&\text{in }\bbr^3,\\ &Δv-(λb(x)+b_0(x))v+μ_2v^3+βu^2v=0\quad&\text{in }\bbr^3,\\ &u,v\in\h,\quad u,v>0\quad\text{in }\bbr^3,\endaligned\right. \end{equation*} where $λ,μ_1,μ_2>0$ and $β<0$ are parameters; $a(x), b(x)\geq0$ are steep potentials and $a_0(x),b_0(x)$ are sign-changing weight functions; $a(x)$, $b(x)$, $a_0(x)$ and $b_0(x)$ are not necessarily to be radial symmetric. By the variational method, we obtain a ground state solution and multi-bump solutions for such systems with $λ$ sufficiently large. The concentration behaviors of solutions as both $λ\to+\infty$ and $β\to-\infty$ are also considered. In particular, the phenomenon of phase separations is observed in the whole space $\bbr^3$. In the Hartree-Fock theory, this provides a theoretical enlightenment of phase separation in $\bbr^3$ for the 2-mixtures of Bose-Einstein condensates.

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Infinitely many sign-changing and semi-nodal solutions for a nonlinear Schrodinger system

We study the following coupled Schrödinger equations which have appeared as several models from mathematical physics: {displaymath} {cases}-Δu_1 +\la_1 u_1 = μ_1 u_1^3+βu_1 u_2^2, \quad x\in Ω, -Δu_2 +\la_2 u_2 =μ_2 u_2^3+βu_1^2 u_2, \quad x\in \Om, u_1=u_2=0 \,\,\,\hbox{on \,$\partial\Om$}.{cases}{displaymath} Here $\Om$ is a smooth bounded domain in $\R^N (N=2, 3)$ or $\Om=\RN$, $\la_1,\, \la_2$, $μ_1,\,μ_2$ are all positive constants and the coupling constant $\bb<0$. We show that this system has infinitely many sign-changing solutions. We also obtain infinitely many semi-nodal solutions in the following sense: one component changes sign and the other one is positive. The crucial idea of our proof, which has never been used for this system before, is turning to study a new problem with two constraints. Finally, when $\Om$ is a bounded domain, we show that this system has a least energy sign-changing solution, both two components of which have exactly two nodal domains, and we also study the asymptotic behavior of solutions as $β\to -\infty$ and phase separation is expected.

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