Boundedness of Hausdorff operators on the power weighted Hardy spaces

In this paper, we consider the two-dimensional Hausdorff operators on the power weighted Hardy space H_(|x|α)~1(R~2) ( -1 ≤α≤0), defined by H_(Φ,A)f(x)=∫R~2Φ(u)f(A(u)x)du,where Φ∈L_loc~1(R~2),A(u) = (α_(ij)(u))_(i,j=1)~2 is a 2×2 matrix, and each α_(i,j) is a measurablefunction.We obtain that HΦ,A is bounded from H_(|x|~α)~1(R~2) ( -1≤α≤0) to itself, if∫R2|Φ(u)‖det A~(-1)(u)|‖A(u)‖~(-α)ln(1+‖A~(-1)(u)‖~2/|det A~(-1)(u)|)du∞.This result improves some known theorems, and in some sense it is sharp.     

椭圆型方程伪域方法的外推计算

在n维空间的有界区域Ω_1上考虑微分方程相应的边界条件是 u(x)=0,x∈?Ω_1。 (1.2)在以下的讨论中,假设对问题(1.1)和(1.2)下述条件成立: (i)所有的α_(ij)(x)在区域Ω_1上一致Lipschtz连续,且α_(ij)(x)=α_(ji)(x),i,j=1,     

退缩椭圆型方程的边值问题

<正> 在 R~n 的有界凸区域Ω上考虑椭圆型方程Lu≡sum from i,j=1 to n (a_(ij)(x)u_(xi)_(xj)+sum from i=1 to n b_i(x)u_i+c(x)u=f(x),(1)设对 x∈(?)及所有的实数组(ξ_1,ξ_2,…,ξ_n)sum from i,j=1 to n a_(ij)(x)ξ_iξ_j≥λ(x)sum from i=1 to n ξ_i~2≥0,a_(ji)(x)∈C(?),即算子 L(u)可能退缩而为退缩椭圆型算子。记(?)的边界为∑,∑上满足 sum from ij=1 to n a_(ij)n_in_j=0的点集为∑_0,(n_1,…,n_n)表示∑上的内单位法向量,∑_3=∑\∑_0,设其 n-1维测度非零,则对方程(1)可提如下的边值问题:     

三维拟线性波方程的小初值光滑解

对三维小初值拟线性波方程3∑(i,j=0)g~(ij)(u)■_(ij)u=0,H.Lindblad证明了它有整体光滑解.本文考虑如下带有小初值的拟线性波方程3∑(i,j=0)g~(ij)(u)■_(ij)u=(■u)~3,通过得到低阶导数的衰减估计和高阶导数的能量估计,由连续论证法证明了这个方程也存在整体光滑解.     

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．     

关于两类线性变时控制系统的一致渐近稳定性

其中,x(t)∈R~n 是状态向量,u(t)∈R~r 是输入向量,A(t)=(a_(ij)(t))_(n×n)是系数矩阵,B(t)=(b_(ij)(t))_(n×r)是输入变量系数矩阵,根据 Lagrange 常数交易公式,系统(1)的解可表为:     

Hammerstein型积分方程组的非零解及其对两点边值问题的应用

本文研究Hammerstein型积分方程组 (Ⅰ)φ(x)=∫_G K_1(x,y)f_1(φ(y),ψ(y))dy, ψ(x)=∫_G K_2(x,y)f_2(φ(y),ψ(y))dy非零解的存在性(其中G为R~N中有界闭区域,mesG=1,并将所得结果应用于二阶常微分方程两点边值问题 (Ⅱ)(t)=-f(x(t),(t)), α_0x(0)-β_0(0)=0, α_1x(1) β_1(1)=0。其中α_0、α_1、β_0、β_1≥0,|α_0 β_0 -α_1 α_1 β_1|≠0。所得结论与[1]第四章及[3]第六章所述结论具有不同形式,且不能用[1、3]的方法得出,特别当f(u,v)是多项式情况下所得结果是[2]中部分结果的推广和补充。     

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.     

拟幂零积分算子

本文讨论积分算子的拟幂零性,对 L~p 空间上的积分算子(If)(x)=∫_0~(φ(x))f(t)dt 和 L~2空间上具有非负核的积分算子(Tf)(x)=∫_0~1K(x,t)f(t)dt,分别得到了用积分上限φ和核 K 表述的、使算子 I 和 T 为拟幂零的充要条件.     

SOME GENERAL RESULTS ON THE FIRST BOUNDARY VALUE PROBLEM FOR QUASILINEAR DEGENERATE PARABOLICE QUATIONS

In this paper,the authors investigate the first boundary value problem for equations ofthe formwithAn existence theorem of solution in BV_(1,1/2)(Q_T)is proved.The principal condition is thatthere exists δ>0 such that for any(x,t)∈Q_T,|u|≤Ma~(ij)(u,x,t)ξ_iξ_j-δ(a_(x_θ)~(ij)(u,x,t)ξ_i)~2≥0.a, ~=1     

Lp-Lq Estimates for a Linear Perturbed Klein-Gordon Equation

We consider L^p-L^q estimates for the solution u(t,x) to tbe following perturbed Klein-Gordon equation ∂_{tt}u - Δu + u + V(x)u = 0 \qquad x∈ R^n, n ≥ 3 u(x,0) = 0, ∂_tu(x,0) = f(x) We assume that the potential V(x) and the initial data f(x) are compact, and V(x) is sufficiently small, then the solution u(t,x) of the above problem satisfies ||u(t)||_q ≤ Ct^{-a}||f||_p for t > 1 where a is the piecewise-linear function of 1/p and 1/q.     

一个局部波动方程组的解的全局存在性与爆破

我们研究初始值问题(e)u1/(e)t2=(e)2u1/(e)x2+‖u2(·,t)‖p, (e)2u2/(e)t2=(e)2u2/(e)x2+‖u1(·,t)‖q,-∞<x<∞,t>0,u1(x,0)=f1(x), (e)u1/(e)t(x,0)=g1(x),u2(x,0)=f2(x), (e)u2/(e)t(x,0)=g2(x),- ∞<x<∞,where‖ui(·,t)‖=∫∞-∞(4)i(x)|ui(x,t)|dx with (4)i(x)≥0 and ∫∞-∞(4)i(x)dx=1,i=1,2.然后建立解的全局存在和爆破的标准,提出爆破增长率.     

MULTIPLE SOLUTIONS FOR THE SCHR?DINGER-POISSON EQUATION WITH A GENERAL NONLINEARITY

We are concerned with the nonlinear Schrodinger-Poisson equation{-△u+(V(x)-λ)u+φ(x)u = f(u),(P)-△ φ = u2,limx|→+∞ φ(x)= 0,x∈ R3,where λ is a parameter,V(x)is an...     

Blow Up in a Semilinear Wave Equation

We consider a semilinear wave equation of the form u_tt(x, t) - Δu(x, t) = - m(x, t)u_t(x, t) + ∇Φ(x) ⋅ ∇u(x, t ) + b(x)|u(x, t)|^{p-2}u(x, t) where p > 2. We show, under suitable conditions on m, Φ, b, that weak solutions break down in finite time if the initial energy is negative. This result improves an earlier one by the author [1].     

具有多项式增长的退缩拟线性抛物变分不等式

考虑拟线性抛物型变分不等式：ｕ∈Ｋａ．ｅ．，〈Ａｕ′，ｖ－ｕ〉∫Ωａｉ（ｘ，ｕ，ｕ）（ｖ－ｕ）ｘｉｄｘ＋∫Ωａ（ｘ，ｕ，ｕ）（ｖ－ｕ）ｄｘ≥０ａ．ｅ．ｔ，ｖ∈Ｋ，这里Ｋ为闭凸集，Ａ为非１—１，可能退缩的线性算子．在ａｉ（ｘ，ｕ，ｐ），ａ（ｘ，ｕ，ｐ）关于ｐ，ｕ具有多项式增长的假设下，得到了正则解的存在性和唯一性．特别是，当Ａ＝Ｉ时，我们便得到文［１０］的结果．     

非线性Klein-Gordon方程柯西问题解的整体存在性与Blow-up

研究非线性Klein-Gordon方程的柯西问题u_(tt)-Δu+u=u|u|~(p-1),x∈R~n,t>0;u(x,0)=u_0(x),u_t(x,0)=u_1(x),x∈R~n.通过引进一族位势井,得到了解的整体存在性与不存在的门槛结果.     

Nontrivial Solutions for Some Semilinear Elliptic Equations with Critical Sobolev Exponents

Let Ω be a bounded domain in R^4(n ≥ 4) with smooth boundary ∂Ω. We discuss the existence of nontrivial solutions of the Dirichlet problem {- Δu = a(x) |u|^{4/(a-2)}u + λu + g(x, u), \quad x ∈ Ω u = 0, \quad x ∈ ∂Ω where a(x) is a smooth function which is nonnegative on \overline{Ω} and positive somewhere, λ> 0 and λ ∉ σ(-Δ). We weaken the conditions on a(x) that are generally assumed in other papers dealing with this problem.     

Entropy Unilateral Solution for Some Noncoercive Nonlinear Parabolic Problems Via a Sequence of Penalized Equations

We give an existence result of the obstacle parabolic equations(b(x,u))/(t)-div(a(x,t,u,▽u))+div(φ(x,t,u))=f in Q_T,where b(x,u) is bounded function of u,the term-div(a(x,t,u,▽u)) is a Leray-Lions type operator and the function φ is a nonlinear lower order and satisfy only the growth condition.The second term f belongs to L~1(Q_T).The proof of an existence solution is based on the penalization methods.     

二维Landau-Lifshitz静态方程组的渐近性质

在本文中，我们讨论了ｕ∧（－Δｕ＋λ（ｕ，ｎ）ｎ）＝０，｜ｕ｜＝１，ｘ∈Ｂ１和ｕ＝（ｘ１，ｘ２，０）ｘ∈Ｂ１的轴对称解ｕλ的渐近行为，其中Ｂ１是Ｒ２中单位圆，ｕ＝（ｕ１，ｕ２，ｕ３）．我们证明了ｕλｕ∞在Ｈ２Ｂ１＼Ｂε，Ｒ３中．     

Existence of Solutions for a Quasilinear Schrödinger Equation with Potential Vanishing

Acta Mathematicae Applicatae Sinica, English Series - We study the following quasilinear Schrödinger equation $$ - \Delta u + V(x)u - \Delta ({u^2})u = K(x)g(u),\,\,\,\,\,\,\,\,x \in...