一类耦合算子矩阵的极大Tseng逆及其在椭圆方程中的应用北大核心CSCD

作者给出了单边耦合算子矩阵的极大Tseng逆具有Banachiewicz-Schur形式的充要条件.作为应用,刻画了具有动态边界条件的椭圆方程{△u=h,在Ω中,-β■u/■v+q△■Ωu-γu=h,在■Ω上的最小范数解,其中Ω■R^(n)是具有光滑边界■Ω的有界域,Δ和Δ■Ω分别是在Ω和■Ω上定义的Laplace(Beltrami)算子,v(x)是在x处的单位外法向量,q,β,γ∈R且q≠0.     

Robin反问题的线性互补解法

正1引言考虑二维Laplace方程的Robin边界问题{△u=0,u∈Ω,?u/?v+pu=g,u∈?Ω=Γ,(1)其中Ω■R~2,Γ表示区域Ω的边界,v(向量)表示Γ上的单位外法向量,Robin系数p是一个非负函数,其支撑Γ_1■Γ,g是给定的函数,其支撑Γ_0■Γ,Γ_0与Γ_1满足Γ_0∩Γ_1=?.这类微分方程产生于一些实际应用,例如模拟电导体和周围环境之间的稳态热传导模型和半导体中金属和硅的接触面模型等,方程中的u,p,g在不同的环境下代表不同的     

一类带临界指数增长的椭圆型方程组两个正解的存在性

该文主要讨论带临界指数的椭圆型方程组{-Δu + a(x)u =2α/α+βuα-1vβ + f(x),x ∈Ω,-Δv+b(x)v=2β/α+βuαvβ-1+ g(x),x ∈ Ω,(*)u ＞ 0,v ＞ 0,x ∈Ω,u=v=0,x ∈(a)Ω解的存在性,其中Ω是RN中一个光滑有界区域,N=3,4,a≥2,β≥2...     

RESEARCH ANNOUNCEMENTS ON“MINIMAL TIME CONTROL OF EXACT SYNCHRONIZATION FOR PARABOLIC SYSTEMS”

正1 Introduction and Main Results LetΩ■R~d (with d≥1) be a bounded domain with a C~2 boundary Ω.Letω■Ωbe an open and nonempty subset with its characteristic function χ_ω.Let A■(a_(ij))_(1≤i,j≤n)∈R~(n×n)and B■(b_(ij))_(1≤i≤n,1≤j≤m)∈R~(n×m) be two constant matrices,where n≥2 and m≥1.Let y_0∈L~2(Ω)~n.Consider the controlled linear parabolic system     

带有流量限制的拟线性趋化模型解的整体有界性

本文考虑如下一类带流量限制的趋化模型:{ut=▽·(up▽u/√u2+|▽u|2)-x▽(uq▽v/√1+|▽v|2),x∈Ω,t＞0,0=△v-μ+u,x∈Ω,t＞0的初边值问题,其中Ω=BR(0)(∈)Rn(n≥2,R＞0),x＞0,μ:=1/|Ω|∫Ωu0(x)dx.本文主要通过区域划分,建立新的先验估计,在p＞...     

拟线性椭圆型问题有限元近似解的迭代加速分析

一、问题的提出 我们考察二阶拟线性椭圆型第一边值问题: -?(α(x,u)?u)=f(x,u),在Ω内, u(x)=0,在?Ω上,其中Ω是R~n(n=2,3)中有界开区域,?Ω是Ω的光滑边界。若u(x),α(x,u(x))和f(x,u(x))有足够正规性,则问题(1)的等价弱形式方程是:对于u∈H_0~1(Ω), (α(x,u)?u,?v)=(f(x,u),v),?v∈H_0~1(Ω)。 (2)这里假设α(x,u)在Ω×R中为正的且有界,内积     

具有阻尼的半线性波动方程解的衰减估计

研究具有阻尼的半线性波动方程的初边值问题u_(tt)-△u+βu_t=|u|~(p-1)u,x∈Ω,t>0u(x,0)=u_0(x),u_t(x,0)=u_1(x),x∈Ωu|_((?)Ω)=0,t≥0其中γ为正常数,Ω■R~n为有界域,当n≥3时,1相似文献   

临界Hartree方程组基态解的存在性（英文）

本文考虑临界耦合的Hartree方程组■其中Ω是R~N中带有光滑边界的有界区域,N≥3,λ,v是常数,且满足λ,v-λ_1(Ω),λ_1(Ω)是(-△,H_0~1(Ω))的第一特征值,β 0是耦合参数,临界指标2_μ~*=(2N-μ)/(N-2)来源于Hardy-LittlewoodSobolev不等式,利用变分的方法证明了临界Hartree方程组基态正解的存在性.     

关于并行迭代区域分解算法的松弛因子

1引言考虑二阶椭圆型Dirichlet边值问题的弱形式,求u∈H_0~1(Ω)使得a(u,v)=(f,v),(?) v∈H_0~1(Ω),(1)其中Ω是平面多角形区域,f∈L~2(Ω),(f,v)=∫_Ωfvdx,a(u,v)=∫_Ω(sum from i,j=1 to 2 a_(ij)(?)u/(?)x_i(?)等 a_0uv)dx,其中[a_(ij)]在Ω上对称一致正定,a_(ij)在Ω上分片连续有界,a_0≥0．由Lax-Milgram引理,问题(1)在H_0~1(Ω)中有唯一解．     

一个带非线性边界条件的强耦合抛物方程组的整体存在性与爆破

本文处理带非线性边界条件 u n=uα, v n=vβ ,(x ,t) ∈ Ω× (0 ,T)的抛物方程组ut =vpΔu ,vt=uqΔv ,(x ,t) ∈Ω× (0 ,T) ,其中Ω RN 为一个有界区域 ,p ,q>0和α ,β≥ 0为常数 .研究了上述问题正解的整体存在性和爆破 ,建立了整体存在和爆破的新标准 .证明了当max{p+β,q+α}≤ 1时正解 (u ,v)整体存在 ,当min{p+β ,q+α}>1且max{α ,β}<1时正解 (u ,v)在有限时刻爆破     

三维弱奇异积分算子的紧性

本文讨论了三维弱奇异核积分算子K:■其中■0α3,■是Ω×Ω上的连续函数.证明了当0α3时,K是从L~1(Ω)空间到L~1(Ω)空间中的紧算子.     

泛函极小与椭圆型方程组解的正则性

研究定义在向量u=(u~1,…,u~N):Ω■R~n→R~N上的各项异性积分泛函F(u)=∫_Ωf(x,Du(x))dx和非线性椭圆型方程组-Σi=1nDi(aiα(x,Du(x)))=-Σi=1nDiFiα(x),α=1,2,…,N.在密度函数f:Ω×R~(N×n)→R和矩阵a=(a_i~α):Ω×R~(N×n)→R~(N×n)满足某单调不等式条件下,得到u整体有界.     

Multiplicity of solutions of weighted (p,q)-Laplacian with small source

In this article, we study the existence of infinitely many solutions to the degenerate quasilinear elliptic system-div(h_1(x)|▽u|~(p-2)▽u)=d(x)|u|~(r-2)u+G_u(x,u,v) in Ω,-div(h_2(x)|▽u|~(p-2)▽v)=f(x)|v|~(s-2)v + G_u(x,u,v) in Ω,u=v=0 on ■Ω where Ω is a bonded domain in R~N with smooth boundary ■Ω,N≥2,1 r p ∞,1 s q ∞; h_1(x) and h_2(x) are allowed to have "essential" zeroes at some points inΩ; d(x)|u|~(r-2)u and f(x)|v|~(s-2)v are small sources with Gu(x,u,v), Gv(x,u,v) being their high-order perturbations with respect to(u,v) near the origin, respectively.     

一类非线性Schrdinger方程的解

本文讨论这样一类非线性Schrdinger方程:其中k,v是常数,v>O;Ω■R~2;u(x,t)是复值未知函数;u_0是初值,已知。 给出1.方程整体解的存在性和解的估计;2.在Ω是R~2中的外区域情况下,当t→∞时解的渐近性。     

Regularity for solutions to anisotropic obstacle problems

For Ω a bounded subset of R n,n 2,ψ any function in Ω with values in R∪{±∞}andθ∈W1,(q i)(Ω),let K(q i)ψ,θ(Ω)={v∈W1,(q i)(Ω):vψ,a.e.and v-θ∈W1,(q i)0(Ω}.This paper deals with solutions to K(q i)ψ,θ-obstacle problems for the A-harmonic equation-divA(x,u(x),u(x))=-divf(x)as well as the integral functional I(u;Ω)=Ωf(x,u(x),u(x))dx.Local regularity and local boundedness results are obtained under some coercive and controllable growth conditions on the operator A and some growth conditions on the integrand f.     

关于Schwarz交替法的收敛因子

§1.Schwarz交替法的收敛因子 我们就二阶自共轭椭圆型方程的Dirichlet问题来讨论.设Ω?R~2为一多边形区域, a(u,v)=(f,v),v∈H_0~1(Ω),f∈H~(-1)(Ω), u∈H_0~1(Ω)是定义在其上的边值问题的变分形式,双线性型时a(·,·)满足     

AN EFFECT ITERATION ALGORITHM FOR NUMERICAL SOLUTION OF DISCRETE HAMILTON-JACOBIBELLMAN EQUATIONS

§1Introduction ConsidertheHamilton-Jacobi-Bellmanequation max1≤v≤m[A(v)u(x)-f(v)(x)]=0,x∈Ω(1.1)withtheboundarycondition u(x)=0,x∈Ω(1.2)whereΩisabounded,smoothdomaininEuclideanspaceRd,d∈N;f(v)(x)aregiven functionsfromC2(Ω);A(v)aresecond-orderuniformlyellipticoperatorsoftheform A(v)=-d i,j=1a(v)ij2xixj+di=1b(v)ixi+c(v).(1.3)Intheaboveexpression(1.3)therearecoefficientsa(v)ij,b(v)i,c(v)∈C2(Ω)satisfying,forall1≤v≤m,a(v)ij(x)=a(v)ji(x),1≤i,j≤d,c(v)≥c0≥0,x∈Ω,a…     

偶数阶调和算子△~(2m)的特征值界的估计

设Ω■R~m,m≥2,是边界充分光滑的有界区域,若正数ι满足下列三条件之一:1.l=2~k;2.l=2_0~(k k_1-1) 2~k_0-1,3.l=2~k_0 k_1-2~k,k=0,1,2,…,k_0,k_1=1,2,…,△~(2l)u-λu=0,x∈Ω,则问题u=аu/аn=…=а~(2l-1)u/аn~(2l-1)=0,x∈аΩ,（n是αΩ的单位外法向）的第n 1个特征值λ_(n 1)有下述隐式和显式表示的界     

一类反应扩散差分方程组及有关的离散生态模型

§1.前言基于生物学中的离散模型,文章[1—5]研究了反应扩散差分方程的性质。反应扩散差分方程组,可由如下定解问题 LU=F(x.U),xΩ,t∈[0,T],Ω■R~n, U(x,t)=H(x,t),x∈■Ω,t∈(0,T],(1.1) U(x.0)=U~0(x),x∈Ω=Ω∩■Ω,     

Asymptotic Expansions of the Heat Kernel of the Laplacian for General Annular Bounded Domains with Robin Boundary Conditions：Further Results

The asymptotic expansions of the trace of the heat kernel θ(t)=∑^∞v=1^exp(-tλv) for small positive t,where {λv} are the eigenvalues of the negative Laplacian -△n=-∑^ni=1(D/Dx^1)^2 in R^2(n=2 or 3),are studied for a general annular bounded domain Ω with a smooth inner boundary DΩ1 and a smooth outer boundary DΩ2,where a finite number of piecewise smooth Robin boundary conditions(D/Dnj γh)Ф=0 on the components Гj(j= 1,...,m) of (DΩ1 and on the components Гj (j=k 1,…,m) of of DΩ2 are considered such that DΩl=U^kj=lГj and DΩ2= U^m=k 1Гj and where the coefficients γj(j=1,...,m) are piecewise smooth positive functions. Some applications of θ(t) for an ideal gas enclosed in the general annular bounded domain Ω are given. Further results are also obtained.