重调和方程非平凡解的存在性

该文主要研究$R^N(N>4)$上重调和方程\begin{eqnarray*}\left\{\begin{array}{ll} \Delta^2 u+\lambda u=\overline{f}(x,u);\\ \lim\limits_{|x|\rightarrow\infty}u(x)=0;\\u\in{H^2}(R^N),\hspace{0.1cm}x\in{R^N } \end{array}\right.\end{eqnarray*}的非平凡解的存在性.为了便于研究,将方程转化为$R^N(N>4)$ 上带有扰动项的重调和方程\begin{eqnarray*}\left\{\begin{array}{ll} \Delta^2 u+\lambda u=f(u)+\varepsilon g(x,u);\\ \lim\limits_{|x|\rightarrow\infty}u(x)=0;\\u\in{H^2}(R^N),\hspace{0.1cm}x\in{R^N } .\end{array}\right.\end{eqnarray*}并运用扰动方法进行研究(其中$f(u)=\lim\limits_{|x|\longrightarrow \infty}\overline{f}(x,u),\varepsilon g(x,u)=\overline{f}(x,u)-f(u),\varepsilon$为任意小常数),证明了在适当条件下上述问题非平凡解的存在性.     

一类带p-Laplacian的Sturm-Liouville型2m点边值问题三个正解的存在性

该文考虑了下面的具一维$p$\,-Laplacian算子的多点边值问题 $ \left\{ \begin{array}{rl} &;\disp (\phi_{p}(x'(t)))'+h(t)f(t,x(t),x'(t))=0,\hspace{3mm}01,~\alpha_{i}>0,~\beta_{i}>0,~0<\sum\limits_{i=1}^{m-1}\alpha_{i}\xi_{i}\leq1,~ 0<\sum\limits_{i=1}^{m-1}\beta_{i}(1-\eta_{i})\leq1,~0=\xi_{0} <\xi_{1}<\xi_{2}<\cdots<\xi_{m-1}<\eta_{1}<\eta_{2}<\cdots<\eta_{m-1}<\eta_{m}=1,~i=1,2,\cdots,m-1.$ 通过运用锥上的不动点定理, 该文得到了至少三个正解的存在性. 有趣的是文中的边界条件是一个新型的Sturm-Liouville型边界条件, 这类边值问题到目前为止还很少被研究.     

一维奇异p-Laplacian方程多解的存在性

该文通过利用Leggett-Williams定理,建立了一维奇异p-Laplacian非线性边值问题(\varphi(u'))'+a(t)f(u)=0,\u'(0)=u(1)=0 (或者u(0)=u'(1)=0),其中\varphi(s)=|s|^{p-2}s, p>1三解的存在性定理,推广并丰富了以往文献的一些结论.     

单位正方形上的一些振荡积分及其应用

设Q²=[0, 1]²是Eulid空间$\R^2$上的单位正方形, ${\mathcal{T}}_{\alpha,\beta}$是如下定义在Schwartz函数类${\mathcal{S}}(\R^3)$上振荡奇异积分算子
${\mathcal{T}}_{\alpha, \beta}f(x,y,z)=\int_{Q^2}f(x-t,y-s,z-t^ks^j)e^{-it^{-\beta_1}s^{-\beta_2}}t^{-1-\alpha_1} s^{-1-\alpha_2}dtds.
$
本文首先建立了该算子的L^p有界性, 然后利用这些结果获得了乘积空间上的一些奇异积分算子的(p, p)有界性.     

无限区间上二阶离散问题的正解

在本文中,通过运用离散的Arzel\''{a}-Ascoli引理和锥上的不动点定理,我们讨论了无限区间上二阶离散Sturm-Liouville边值问题$$\left\{\begin{array}{l}\Delta^{2}u(x-1)=f(x,u(x),\Delta u(x-1)),~~x\in\mathbb{N},\\ u(0)-a\Delta u(0)=B,~~\Delta u(\infty)=C\end{array}\right.$$ 正解的存在性,其中$\Delta u(x)=u(x+1)-u(x)$是前向差分算子,$\mathbb{N}=\{1,2,\ldots,\infty\}$且$f:\mathbb{N}\times\mathbb{R_{+}}\times\mathbb{R_{+}}\to\mathbb{R_{+}}$连续,$a>0, B, C$ 为非负实数,$\mathbb{R_{+}}=[0,+\infty)$, $\Delta u(\infty)=\lim_{x\rightarrow\infty}\Delta u(x)$.     

在Banach空间中推广的 Roper-Suffridge算子(III)

假定 $X$ 是具有范数$\|\cdot\|$的复 Banach 空间, $n$ 是一个满足 $\dim X\geq n\geq2$的正整数. 本文考虑由下式定义的推广的Roper-Suffridge算子 $\Phi_{n,\beta_2, \gamma_2, \ldots , \beta_{n+1}, \gamma_{n+1}}(f)$: \begin{equation} \begin{array}{lll} \Phi _{n, \beta_2, \gamma_2, \ldots, \beta_{n+1},\gamma_{n+1}}(f)(x) &;\hspace{-3mm}=&;\hspace{-3mm}\dl\he{j=1}{n}\bigg(\frac{f(x^*_1(x))}{x^*_1(x)})\bigg)^{\beta_j}(f''(x^*_1(x))^{\gamma_j}x^*_j(x) x_j\\ &;&;+\bigg(\dl\frac{f(x^*_1(x))}{x^*_1(x)}\bigg)^{\beta_{n+1}}(f''(x^*_1(x)))^{\gamma_{n+1}}\bigg(x-\dl\he{j=1}{n}x^*_j(x) x_j\bigg),\nonumber \end{array} \end{equation} 其中 $x\in\Omega_{p_1, p_2, \ldots, p_{n+1}}$, $\beta_1=1, \gamma_1=0$ 和 \begin{equation} \begin{array}{lll} \Omega_{p_1, p_2, \ldots, p_{n+1}}=\bigg\{x\in X: \dl\he{j=1}{n}| x^*_j(x)|^{p_j}+\bigg\|x-\dl\he{j=1}{n}x^*_j(x)x_j\bigg\|^{p_{n+1}}<1\bigg\},\nonumber \end{array} \end{equation} 这里 $p_j>1 \,( j=1, 2,\ldots, n+1$), 线性无关族 $\{x_1, x_2, \ldots, x_n \}\subset X $ 与 $\{x^*_1, x^*_2, \ldots, x^*_n \}\subset X^* $ 满足 $x^*_j(x_j)=\|x_j\|=1 (j=1, 2, \ldots, n)$ 和 $x^*_j(x_k)=0 \, (j\neq k)$, 我们选取幂函数的单值分支满足 $(\frac{f(\xi)}{\xi})^{\beta_j}|_{\xi=0}= 1$ 和 $(f''(\xi))^{\gamma_j}|_{\xi=0}=1, \, j=2, \ldots , n+1$. 本文将证明: 对某些合适的常数$\beta_j, \gamma_j$, 算子$\Phi_{n,\beta_2, \gamma_2, \ldots, \beta_{n+1}, \gamma_{n+1}}(f)$ 在$\Omega_{p_1, p_2, \ldots , p_{n+1}}$上保持$\alpha$阶的殆$\beta$型螺形映照和 $\alpha$阶的$\beta$型螺形映照.     

On the Initial-Boundary Value Problems for Quasilinear Symmetric Hyperbolic System with Characteristic Boundary

In this paper we discuss the initial-boundary value problems for quasilinear symmetric hyperbolic system with characteristic boundary.Suppose \Omega is a bounded domain,its boundary \partial \Omega is sufficiently smooth.We consider the quasilinear symmetric hyperbolic system $[\sum\limits_{i = 0}^n {{\alpha _i}(x,u)\frac{{\partial u}}{{\partial {x_i}}}} = f(x,u)\]$ in the domain [0, h]*\Omega. The initial-boundary conditions are $u|_x_0=0$(2) $Mu|_[0,h]*\partial \Omega=0$(3) (No loss of generality, the initial condition may be considered as homogeneous one) . We assume the coefficients of (1), (3) are sufficiently smooth, the compatibility condition and the following conditions are satisfied. 1) when t = 0, u=0, the $\alpha_0(x,u)$ is a positive definite matrix. 2) If [\tilde u\] denotes any vector function satisfying the condition (3), the boundary [0,h]*\partial \Omega is non-characteristic or regular oliarabterigitic for the operator $[\sum\limits_{i = 0}^n {{\alpha _i}(x,\tilde u) \times \frac{\partial }{{\partial {x_i}}}} \]$. and if $v(0,v_1,\cdots,v_n)$ denotes the normal direction to the boundary, the matrix $\beta(x,\tilde u\)=\sum\limits_{i=0}^n v_i \alpha_i(x,\tilde u\)$ is equal to \beta_0, which only depends on x, and Mu=0 is a maximum non-negatiye subspace of quahratio form u\beta_0u. 3) There exists a non-singular matrix Q (x), such that the matrix $\tilde =beta(x,v)=Q'(x)\beta(x,Q^-1v)Q(x)$ may be reduced to a block diagonal matrix $[\left( {\begin{array}{*{20}{c}} {{B_1}}&0\0&{{B_2}} \end{array}} \right)\]$ and the boundary condition may be reduced to $v_1=\cdots=v_L=0$(4) when (t,x) lies on the boundary [0,h] \times \partial \Omega, and v satisfies (4),the block B_1 will be equal to a non-singular matrix B_10 and B_2 will vanish. Under these assumptions, we have proved: Theorem I. There exists a sufficiently small number \delta, such that if h \leq \delta, the local smooth solution of the initial-boundary value problem (1)—(3) uniquely exists. This theorem has been applied to gas dynamics. For both steady flow and unsteady flow in three dimentional space we can use Theorem I to obtain the result of the unique existance of local smooth solution for the correponding system of equations, if there isn;t any shook wave.     

一类二阶奇异微分方程正解的存在唯一性

利用上下解方法,不动点理论研究奇异微分方程u" f(t,u)=0,t∈(0,1)在边界条件au(0)-βu'(0)=0,γu(1) δu'(1)=0下C[0,1]正解和C1[0,1]正解的存在性与唯一性.其中非线性项f(t,u)关于u是减的,仅满足较弱的要求.     

超线性非线性Sturm-Liouville边值问题的正解

利用拓扑方法讨论了一类非线性Sturm-Liouville边值问题{-u″=λf(x,u),0≤x≤1,α0u(0)+β0u′(0)=0, α1u(1)+β1u′(1)=0.研究了上述问题的正解的全局结构,在非线性项f(x,u)不满足条件f(x,u)≥0(u≥0)时获得了正解的存在性.     

一维$P$-Laplace二阶差分系统奇异边值问题正解的存在性

应用锥压缩锥拉伸不动点定理和Leray-Schauder 抉择定理研究了一类具有P-Laplace算子的奇异离散边值问题$$\left\{\begin{array}{l}\Delta[\phi (\Delta x(i-1))]+ q_{1}(i)f_{1}(i,x(i),y(i))=0, ~~~i\in \{1,2,...,T\}\\\Delta[\phi (\Delta y(i-1))]+ q_{2}(i)f_{2}(i,x(i),y(i))=0,\\x(0)=x(T+1)=y(0)=y(T+1)=0,\end{array}\right.$$的单一和多重正解的存在性,其中$\phi(s) = |s|^{p-2}s, ~p>1$,非线性项$f_{k}(i,x,y)(k=1,2)$在$(x,y)=(0,0)$具有奇性.     

弱半正三阶三点边值问题的正解

The positive solutions are studied for the nonlinear third-order three-point boundary value problem u′″（t）=f（t,u（t））,a.e,t∈[0,1],u（0）=u′（η）=u″（1）=0, where the nonlinear term f（t, u） is a Caratheodory function and there exists a nonnegative function h ∈ L^1[0, 1] such that f（t, u） 〉 ≥-h（t）. The existence of n positive solutions is proved by considering the integrations of ＂height functions＂ and applying the Krasnosel＇skii fixed point theorem on cone.     

一类非线性$m$-点边值问题的正解

应用锥理论和不动点指数方法,在与相应线性算子的第一特征值相关的条件下,得到了下述非线性二阶常微分方程m-点边值问题{u"(t) a(t)u' b(t)u h(t)f(u(t))=0,0＜t＜1,u'(0)=0,u(1)=m-2∑i=1αiu(ξi).的正解,改进了相关文献中的结论.     

一类二阶常微分方程边值问题的无穷多个解

利用变分原理和Z2不变群指标研究了二阶常微分方程边值问题{u″(t)-u(t) f(t,u(t))=0,0＜t＜1,u′(0)=0,α1u(1) u′(1)=0,(其中α1＞-1/2).得出了这类方程存在无穷个解的充分条件.     

一类奇异三阶三点边值问题的正解

In this paper,we study the existence of positive solutions for the nonlinear singular third-order three-point boundary value problemu （t） = λa（t）f（t,u（t））,u（0） = u （1） = u （η） = 0,where λ is a positive parameter and 0 ≤ η 1 2 .By using the classical Krasnosel’skii’s fixed point theorem in cone,we obtain various new results on the existence of positive solution,and the solution is strictly increasing.Finally we give an example.     

On the existence of positive solutions of nonlinear second order differential equations

Under suitable conditions on , the boundary value problem

has at least one positive solution. Moreover, we also apply this main result to establish several existence theorems of multiple positive solutions for some nonlinear (elliptic) differential equations.

     

Positive solutions for system of 2n-th order Sturm–Liouville boundary value problems on time scales

Intervals of the parameters λ and μ are determined for which there exist positive solutions to the system of dynamic equations $$ \begin{array}{lll} && (-1)^nu^{\Delta^{2n}}(t)+\lambda p(t)f(v(\sigma(t)))=0,\quad t\in[a, b], \\ &&(-1)^n v^{\Delta^{2n}}(t)+\mu q(t)g(u(\sigma(t)))=0, \quad t\in[a, b], \end{array} $$ satisfying the Sturm–Liouville boundary conditions $$ \begin{array}{lll} &&\alpha_{i+1} u^{\Delta^{2i}}(a)-\beta_{i+1} u^{\Delta^{2i+1}}(a)=0,\;\gamma_{i+1} u^{\Delta^{2i}}(\sigma(b))+\delta_{i+1} u^{\Delta^{2i+1}}(\sigma(b))=0,\\ &&\alpha_{i+1} v^{\Delta^{2i}}(a)-\beta_{i+1} v^{\Delta^{2i+1}}(a)=0,\; \gamma_{i+1} v^{\Delta^{2i}}(\sigma(b))+\delta_{i+1} v^{\Delta^{2i+1}}(\sigma(b))=0, \end{array} $$ for 0?≤?i?≤?n???1. To this end we apply a Guo–Krasnosel’skii fixed point theorem.     

Solvability of a Kind of Sturm–Liouville Boundary Value Problems with Impulses via Variational Methods

The purpose of this paper is to use a three critical point theorem due to Ricceri to obtain the existence of at least three solutions for the following Sturm–Liouville boundary value problem with impulses

$\begin{cases}(\phi_{p}(x'(t)))'=(a(t)\phi_{p}(x)+\lambda f(t,x)+\mu h(x))g(x'(t)),\quad \mbox{a.e. }t\in[0,1],\\\Delta G(x'(t_{i}))=I_{i}(x(t_{i})),\quad i=1,2,\ldots,k,\\\alpha_{1}x(0)-\alpha_{2}x'(0)=0,\\\beta_{1}x(1)+\beta_{2}x'(1)=0,\end{cases}$

where p>1, φ _p (x)=|x|^p?2 x, λ, μ are positive parameters, \(G(x)=\int_{0}^{x}\frac{(p-1)|s|^{p-2}}{g(s)}\,ds\). The interest is that the nonlinear term includes x′. We exhibit the existence of at least three solutions and h(x) can be an arbitrary C ¹ functional with compact derivative. As an application, an example is given to illustrate the results.

     

四阶奇异边值问题的正解

研究了一类四阶奇异边值问题正解的存在性,在f和g满足比超线性和次线性条件更广泛的极限条件下,利用锥压缩和拉伸不动点定理获得了正解的存在性结果,推广和包含了一些已知结果.