Existence of solutions for fourth-order boundary value problem with parameter

This paper is a sequel to a previous paper (Yang,Y.and Zhang,J.H.Existence of solutions for some fourth-order boundary value problems with parameters.Nonlinear Anal.69(2),1364–1375 (2008)) in which the nontrivial solutions to the fourthorder boundary value problems were studied.In the current work with the same conditions near infinity but different near zero,the positive,negative,and sign-changing solutions are obtained by the critical point theory,retracting property,and invariant sets.     

一类拟线性椭圆方程的非平凡解

运用环绕理论和对称型山路理论对一类具有次临界多项式增长和次临界指数增长的$p$-Laplacian方程建立一个非平凡解(无穷多个非平凡解)的存在性结果.     

Positive solutions of three-point boundary value problems

In this paper, we consider existence of single or multiple positive solutions of three-point boundary value problems involving one-dimensional p-Laplacian. We then study existence of solutions when the problems are in resonance cases. The proposed approach is based on the Krasnoselskii＇s fixed point theorem and the coincidence degree.     

Heisenberg群上半线性Kohn-Laplace′s方程的Dirichlet问题

本文用上下解方法,获得半线性次椭圆方程Dirichlet问题的-些存在性结果.     

关于极小极大原理

通过减弱条件,获得了一个新的结果。由此,我们给出一些新的极小极大定理和极小极大不等式。     

具有不定位势和凹非线性项的Robin问题的解的多重性

研究非线性项由凹项λ|u|^q?2(其中1相似文献   

三点边值问题的正解

利用Krasnoselskii's不动点定理和重合度定理,研究了p-Laplace三点边值问题单解或多解的存在性,以及在共振情况下解的存在性.     

Heisenberg群上半线性方程解的非存在性定理

本文利用Rellich恒等式建立了Heisenberg群上一类半线性方程解的非存在性结果．     

Heisenberg群上非线性方程的存在性结果

本文通过变分方法给出了Ｈｅｉｓｅｎｂｅｒｇ 群上非线性方程的存在性结果     

Existence Results for Nonlinear Subelliptic Equations on the Heisenberg Group

§ 1.Introduction　 The aim of this paper is to establish existence results,by monotone method,for theproblemΔHnu + f((z,t) ,u) =0　　 in D,u| D =0 (1 .1 )where D is an open subset of the Heisenberg group HnandΔHn is the subelliptic Lapla-cian on Hn.We recall that Hnis the Lie group whose underlying manifold is Cn× R,n∈N,endowed with the group law(z,t) (z′,t′) =(z + z′,t+ t′+ 2 Imz .z′) ,(1 .2 )where for z,z′∈ Cnwe have letz .z′= nj=1zjz′j.Set zj=xj+ iyj.Then (x1 ,… ,xn…