一类奇异非线性三点边值问题的正解

应用锥上的不动点定理，建立了奇异非线性三点边值问题(u″(t)+a(t)f(u)=0,0＜t＜1,αu(0)-βu′(0)=0,u(1)-ku(η)=0)正解的一个存在性定理．这里η∈(0,1)是一个常数，a∈C( (0,1),［0,+∞)),f∈C(［0,+∞),［0,+∞))     

Robin型二阶m 点边值问题正解的存在性

设 a∈C［0,1］, b∈C(［0,1］,(-∞, 0)). 设\-1(t)为线性边值问题  u″+a(t)u′+b(t)u=0， u′(0)=0,\ u(1)=1  的唯一正解. 该文研究非线性二阶常微分方程m 点边值问题  u″+a(t)u′+b(t)u+h(t) f(u)=0，\= u′(0)=0, u(1)-∑[DD(]m-2[]i=1[DD)]α\-i u(ξ\-i)=d  正解的存在性. 其中 d 为参数, ξ\-i∈(0,1), α\-i∈(0,∞) 为满足 ∑[DD(]m-2[]i=1[DD)]α\-i\-1(ξ\-i)<1的常数, i∈{1,\:，m-2}. 在适当的条件下证得: 存在正常数 d\+*, 使 当0d\+*时无正解.     

非线性二阶微分系统正解的存在性

考虑二阶微分系统边值问题[JB({]x″(t)+λ f(t,x(t),y(t))=0,\=y″(t)+μ g(t,x(t),y(t))=0,\ 00, f, g:［0,1］×［0,∞)×［0,∞)→R连续. 突破了以往文献要求非线性项 f, g非负的限制，运用锥上的一个不动点定理,在半正的情形下建立了问题正解的存在性     

二阶常微分方程无穷多点边值问题的正解

该文运用锥上的不动点定理研究非线性二阶常微分方程无穷多点边值问题 u'+a (t ) f (u)=0, t∈(0, 1), u(0)=0, u(1)=∑^∞_{i =1}α _i u ( ξ _i ) 正解的存在性. 其中ξ _i∈ (0,1),α _i∈ [0,∞), 且满足∑^∞_i=1α_iξ _i <1.α∈C([0,1], [0,)),f∈C ([0,∞), [0,∞)).     

一类两点边值问题的多重非负解

该文考虑两点边值问题[1/q(t)][q(t)y′(t)]′+p(t)f(y(t))= 0,λ_1 y(α)-λ_2y′(α)=0 and y(β)=B非负解的存在性, 其中p(t)可能在t=α或t=β附近具有奇异性, f(0)≥0, lim_(y→+∞)f(y)/y=+∞, 并且存在y>0, 使得f(y)<0.      

半无穷区间广义Sturm-Liouville边值问题的多个正解存在性

该文利用Leggett-Williams 不动点定理, 研究半无穷区间边值问题 (p(t)x'(t))'+Φ(t) f (t, x(t), x'(t))=0, t∈[0,+∞), α₁x(0)-β₁lim_t→0⁺ p(t) x'(t)=a₁, α₂lim_t→+∞ x'(t)+β₂lim_t→+∞ p(t) x'(t)=a₂. 多个正解的存在性.     

多维非退化扩散过程的象集与图集的一致Hausdorff维数

设X(t)=X(0)+∫^t_0α(X(s))dB(s)+∫^t_0β( X(s))ds为一d(d≥3)维非退化扩散过程。令X(E)={X(t): t∈E}, GRX(E)={(t,X(t)): t∈E}，该文证明了：对几乎所有ω：E B([0,∞)),有dimX(E,ω)=dimGRX(E,ω)=2dimE,这里dimF表示F的Hausdorff维数。     

拟线性抛物方程的弱解

该文给出了拟线性退化抛物方程pa_t{u}+pa_x{f(u)}=pa_xx{A(u(x,t))}∈R^2_+×(0,+∞) ,u(x,0)=u_0(x),x∈R 一种弱解的新定义, 利用Div Curl引理证明了解的存在性．     

一类非线性m-点边值问题正解的存在性

设α∈C[0,1],b∈C([0,1],(-∞,0)).设φ(t)为线性边值问题 u″+a(t)u′+b(t)u=0, u′(0)=0,u(1)=1的唯一正解.本文研究非线性二阶常微分方程m-点边值问题 u″+a(t)u′+b(t)u+h(t)f(u)=0, u′(0)=0,u(1)-sum from i=1 to(m-2)((a_i)u(ξ_i))=0正解的存在性.其中ξ_i∈(0,1),a_i∈(0,∞)为满足∑_(i=1)~(m-2)a_iφ_1(ξ_i)<1的常数,i∈{1,…,m-2}.通过运用锥上的不动点定理,在f超线性增长或次线性增长的前提下证明了正解的存在性结果.     

非线性奇异微分方程边值问题的正解

本文的主要结果为：若f(t,u):(0,1)×(0,+∞→[0,+∞）连续,关于u单调减少,存在实数b＞0使对任意0＜r＜1有（0,1）×（0,∞）,则奇异二阶边值问题有正解的充要条件为,有C1[0,1]正解的充分必要条件为其中α,β,σ,γ是非负实效,且为所述边值问题的Green函数．     

The Stokes and Krasovskii Conjectures for the Wave of Greatest Height

The integral equation:
φ_μ(s) = (1/3 π)∫^π ₀((sin φ_μ(t))/(μ ⁻¹+ ∫^t ₀sin φ_μ(u) d u )) (log((sin½( s + t ))/ (sin½( s − t )))d t
was derived by Nekrasov to describe waves of permanent form on the surface of a nonviscous, irrotational, infinitely deep flow, the function φ_μ giving the angle that the wave surface makes with the horizontal. The wave of greatest height is the singular case μ=∞, and it is shown that there exists a solution φ_∞ to the equation in this case and that it can be obtained as the limit (in a specified sense) as μ→∞ of solutions for finite μ. Stokes conjectured that φ_∞( s )→⅙π as s ↓0, so that the wave is sharply crested in the limit case; and Krasovskii conjectured that sup _{s ∈[0,π]}φ_μ( s )≤⅙π for all finite μ. Stokes' conjecture was finally proved by Amick, Fraenkel, and Toland, and the present article shows Krasovskii's conjecture to be false for sufficiently large μ, the angle exceeding ⅙π in what is a boundary layer.     

Jacobian-determinant equation in the critical Besov spaces

Let Ω be a bounded domain in R~n with smooth boundary. Here we consider the following Jacobian-determinant equation det u(x)=f(x),x∈Ω;u(x)=x,x∈?Ω where f is a function on Ω with min_Ω f = δ 0 and Ωf(x)dx = |Ω|. We prove that if f ∈B_(p1)~(np)(Ω) for some p∈(n,∞), then there exists a solution u ∈ B_(p1)~(np+1)(Ω)C~1(Ω) to this equation. On the other hand, we give a simple example such that u ∈ C_0~1(R~2, R~2) while detu does not lie in B_(p1)~(2p)(R~2) for any p∞.     

关于奇异非线性多调和方程的正整体解

该文主要研究形如Δ((Δ\+nu)\+\{p-1*\}) = f(|x|, u, |u|)u\+\{-β\},\ x∈R\+2的奇异非线性多调和方程在R\+2上的正整体解，此处p>1，β≥0是常数，n是自然数，f: [AKR-]\-+×R\-+×[AKR-]\-+→R\-+是 一个连续函数,ξ\+\{α*\}:=|ξ|\+\{α-1\}ξ,ξ∈R，α>0 . 证明了这种解 u必无界且其渐进阶（当n→∞时u作为无穷大量的阶）不低于|x|\+\{2n\}log|x| ，给 出了该方程具有无穷多个其渐进阶刚好为 |x|\+\{2n\}log|x| 的正整体解的充分与充分必要条件. 这些结论可以推广到更一般的方程中去.      

TWO POSITIVE SOLUTIONS TO THREE-POINT SINGULAR BOUNDARY VALUE PROBLEMS

In this article, we consider the existence of two positive solutions to nonlinear second order three-point singular boundary value problem: -u′′(t) = λf(t, u(t)) for all t ∈ (0, 1) subjecting to u(0) = 0 and αu(η) = u(1), where η∈ (0, 1), α∈ [0, 1), and λ is a positive parameter. The nonlinear term f(t, u) is nonnegative, and may be singular at t = 0, t = 1, and u = 0. By the fixed point index theory and approximation method, we establish that there exists λ* ∈ (0, +∞], such that the above problem has at least two positive solutions for any λ∈ (0, λ*) under certain conditions on the nonlinear term f.     

关于亚纯代数体函数的奇异方向

设T(r, w)满足:lim_{r →∞}lg T(r, w)/lg r =0,lim_r→∞lg T(r, w)/lg lg r =+ ∞, 则一定存在一条方向arg z=θ₀ ,使对任意给定N>0,任意复数 a (至多有2 v个例外值), 有∑_i1/(lg|z_i(a;?(θ₀,δ))|)^N=∞.设T(r, w)满足:lim_r→∞T(r, w)/lg^Kr =+∞,lim_r→+∞lg T(r, w) /lg lg r =M, 则一定存在一条方向argz=θ₀ ,对任意复数a (至多有2 v个例外值),有∑_i1/lg|z_i(a;?(θ₀,δ))|)^σ=∞(σ = M-2或σ = M-2-ε.即使在亚纯函数,这些奇异方向也未见研究.     

Asymptotic Expansions for Two Singularly Perturbed Convection–Diffusion Problems with Discontinuous Data: The Quarter Plane and the Infinite Strip

We consider a singularly perturbed convection–diffusion equation,     , defined on two domains: a quarter plane,  ( x , y ) ∈ (0, ∞) × (0, ∞)  , and an infinite strip,  ( x , y ) ∈ (−∞, ∞) × (0, 1)  . We consider for both problems discontinuous Dirichlet boundary conditions:   u ( x , 0) = 0  and   u (0, y ) = 1  for the first one and   u ( x , 0) =χ_{[ a , b ]}( x )  and   u ( x , 1) = 0  for the second. For each problem, asymptotic expansions of the solution are obtained from an integral representation in two limits: (a) when the singular parameter  ε→ 0⁺  (with fixed distance r to the discontinuity points of the boundary condition) and (b) when that distance   r → 0⁺  (with fixed ε). It is shown that in both problems, the first term of the expansion at  ε= 0  is an error function or a combination of error functions. This term characterizes the effect of the discontinuities on the ε-behavior of the solution and its derivatives in the boundary or internal layers. On the other hand, near the discontinuities of the boundary condition, the solution u ( x , y ) of both problems is approximated by a linear function of the polar angle at the discontinuity points.