任意阶Laplace算子的特征值估计

设D为n维Euclid空间Rn的一个有界区域,且0＜λ1≤λ2≤…≤λk≤…是l阶Laplace算子的Dirichlet问题{(-△)lu=λu, 在D中,u=(e)u/(e)n=…=(e)l-1u/(e)nl-1=0,在(e)D上的特征值.得到了该问题用其前k个特征值来估计第(k+1)个特征值λk+1的不等式k∑i=1(λk+1-λi)≤1/n(4l(n+2l-2)]1/2{k∑i=1(λk+1-λi)1/2λil-1/lk∑i=1(λk+1-λi)1/2λi1/l}1/2,此不等式不依赖于区域D.对l≥3,上述不等式比所有已知的结果都要好.陈庆民与杨洪苍考虑了l=2的情形.我们的结果是他们结果的自然推广.当l=1时,我们的不等式蕴含杨洪苍不等式的弱形式.文中还给出了陈和杨的一个断言的直接证明.     

Hardy-Hilbert型不等式的一个加强

改进了Hlder不等式,并利用加强的Hlder的不等式对联系β函数的带参数的Hardy-Hilbert型不等式进行了改进,建立一个新的形如sum from n=1 to ∞ sum from m=1 to ∞(ambn/(m+n)λ)/相似文献   

一类Y~(SG)(γλ,n)∪βS_n~G形图簇的伴随分解及其补图的色等价性

设G是m阶连同图,我们用S_n~G(n=km+1)表示把kG的每个分支的d_i度点分别与星图S_k+1的k个1度点重迭后得到的图,Y~(SG)(r_1n,n)表示把r_1S_n~G中每个分支的k度点依次与图的k度点邻接后得到的图,Y~(SG)(r_2λ_1,n)表示把τ_2Y~(SG)(τ_1n,n)中每个分支的r_1+k度点依次与图S_n~G的k度点邻接后得到的图,若k≥3,用Y~(sG)(r_kλ__(k-1),n)表示把τ_kY~(sG)(r_(k-1)λ_(k-2),n)中每个分支的τ_(k-1)+k度顶点依次与图S_n~G的k度点邻接后得到的图,这里λ_k=r_kλ_(k-1)+n.运用图的伴随多项式的性质,证明了一类新的图簇Y~(sG)(r_kλ__(k-1),n)∪β_kS_n~G的伴随多项式的因式分解定理,进而得到了这类图的补图的色等价图.     

Bargmann空间中无界Gribov-Intissar算子的谱逼近（英文）

在[Adv.Math.(China),2015,44(3):335-353]中,我们研究了经典Bargmann空间Bo中的非自伴算子H_μ:H_μ=S_μ+H_λ,其中S_μ=μz d/(dz),H_λ=iλ(z(d~2)/(dz~2)+z~2 d/(dz)),i~2=-1,参数μ,λ都是实数.我们给出了H_μ的谱分析和H_μ的广义特征向量的渐近分析.设ek(z)=(z~k)/((k!)~(1/2)),k=1,2,…是B0的正交基.算子H_μ可以被一列三对角矩阵逼近,此三对角矩阵的主对角线元素为β_k=μk,次对角线元素α_k=iλk(k+1)~(1/2),1≤k≤n,n∈N.对于μ∈C和λ∈C,本文主要研究上述矩阵的特征值z_(k,n)(μ,λ)的局部化,它是多项式P_(n+1)~(μ,λ)(z)的零点,P_(n+1)~(μ,λ)(z)满足三项递推关系:若"∈R和λ∈R,则上述矩阵是复对称的.在这种情况下,我们证明了R上有界变分复值函数∈(z)的存在性,它使得权重为∈(z)的多项式P_n~(μ,λ)(z)是正交的.我们也考虑了H_μ的扰动H_λ'=S_λ'+H_λ,其中S_λ'=λ'z~2(d~2)/(dz~2)+S_μ,λ'∈R,H_λ可以被矩阵(h_(jk)~λ)_(j,k=1)~∞表示.证明了可以通过S_λ'的特征值和有限矩阵(h_(jk)~λ)_(j,k=1)~n的特征值的组合来逼近H_λ'的特征值.     

单位球上Yamabe方程的全局分歧

该文研究了N维单位球面S^N上的Yamabe方程■通过分歧的方法,对于任意k≥1,证明了该方程对于任意的λ>λ_k:=(k+N-1)(N-2)/4都至少有一个非常数解v_k,使得v_k-λ⁽1/(N*-1))正好有k个零点,并且它们在(-1,1)中都是单根,其中N^*是Sobolev临界指数.在应用部分,得到了当n≥4时,R^N上非线性椭圆方程非径向解的存在性.此外,还得到了乘积流形中一个流形是单位球时的Yamabe问题的全局分歧结果.     

一个含参数根式不等式链

文[1]给出了如下含参数根式不等式:定理1设ai∈R ,i=1,2,…,n,且∑ni=1ai=k,λ>0,μ≥0,则λk μ (n-1)μ0,μ≥0,则λk μn2≤n∑i=1λkai2 μ<λk μ (     

一类非线性微分方程周期解及全局稳定性

本文研究下面一类非线性微分方程dsdt=1 -s- x1 s0 δQ2 ( m1 s0 sk1 s0 s-k)dx1 dt =x1 Q( m1 s0 sk1 s0 s-k) -x1 -x2m2 x1 /Qk2 x1 /Qdx2dt =x2Qm2 x1 /Qk2 x1 /Q -x2　　如果条件m2 x 2 (k1 δ s0 δ-Qλ2 -x 2 ) 2 >m1 δk1 (k2 Q2 λ2 ) 2成立时 ,系统在Ω内存在周期解 ;如果条件m2 x 2 (k1 δ s0 δ -Qλ2 -x 2 ) 2 相似文献   

关于完备λ超曲面的第二拼挤定理

欧氏空间R~(n+1)中满足方程H=-X~N+λ的浸入超曲面称为λ超曲面.本文主要研究欧氏空间中完备λ超曲面的第二拼挤问题.设M为R~(n+1)中具有多项式体积增长的n维完备λ超曲面.设M的第二基本形式为A.本文证明存在正的绝对常数γ,如果|λ|≤γ,β_λ≤|A|~2≤β_λ+~1/21,其中β_λ=1/2(2+λ~2+|λ|(λ~2+4)~1/2),那么|A|~2≡β_λ,λ≥0,且M必为n维球面S~n(n~1/2)、n维圆柱面S~k(k~1/2)×R~(n-k)(1≤ k≤ n-1)或S(((λ2+4)~1/2-|λ|)/2)×R~(n-1)之一.     

几类半线性椭圆共振问题

设Ω∪→R^n是一个有界正则区域，{λk}是－△在H0（Ω）上的一列特征值。假定对某个给定的k，λk是单重的，φ为其相应的特征函数，∫φ^2=1，固定h∈H^-1使∫hφ=0。对于方程（P1）{－△u-λu g（x，u）=tφ h，u=0。σΩ本文利用连通技巧和闭联集理论，推广了文[1]、[3]、[4]中的一些结果。我们获得定理1 假设g:R^*→R满足（g1）g是具有周期原函数的连续周期函数，λk（k≥）简单。如果对任意s ∈R，有（H′4{λk-1≤λ g′（s）≤λk 1k＞1。const≤λ g′（s）≤λ2。则任意h∈H^1,E←τ1,τ2∈R。τ1≤0≤τ2使（i）（P1）有解当且仅当t∈[τ1,τ2]。(ii)如果t∈[τ1,τ2]－{0}，则（P1）至少有两个不同的解。定理2 假设（H′4）成立，λk简单，g满足（H2）任意s，g按x在Ω上可测；g∈C^1对a.e.x∈Ω。（H5）g有界limsg(x,s)=μ＞0。|s|→∞则任意h∈H′0, E←τ1,τ2∈R，τ1＜0＜τ2使（i）（P1）有解当且仅当t∈[τ1,τ2]。（ii）若t∈[τ1,τ2]－{0}，则（Pt）至少有两个不同的解。定理3 [3,prop.2.4]中的条件q＜v（-△-λkI）换成q≤v（-△-λkI）结论仍然成立。     

任意阶Laplace拉普拉斯算子的特征值估计

设D为n维Euclid空间Rⁿ的一个有界区域,且0<λ₁≤λ₂≤…≤λ_k≤…是l阶Laplace算子的Dirichlet问题的特征值．得到了该问题用其前k个特征值来估计第(k+1)个特征值λk+1的不等式此不等式不依赖于区域D．对l≥3,上述不等式比所有已知的结果都要好．陈庆民与杨洪苍考虑了l=2的情形．我们的结果是他们结果的自然推广．当2=1时,我们的不等式蕴含杨洪苍不等式的弱形式．文中还给出了陈和杨的一个断言的直接证明．     

A simple heuristic for the p-centre problem

We describe a simple heuristic for determining the p-centre of a finite set of weighted points in an arbitrary metric space. The computational effort is O(np) for an n-point set. We show that the ratio of the objective function value of the heuristic solution to that of the optimum is bounded by min(3, 1 + α), where α is the maximum weight divided by the minimum weight of points in the set.     

双退缩抛物型方程解的一个性质

在Ｑ＝Ｇ×（０，Ｔ）考虑一类双退缩抛物型方程，在满足较一般的结构条件下，证明了如果它的解在抛物边界等于零，那么必是平凡解．     

一个一维半导体简化能量输运模型的稳态解

在一维空间中分析带有Dirichlet边界条件的半导体简化能量输运稳态方程组,在某些条件下证明了其古典解的存在性.证明基于对电子密度的漂移扩散型方程的仔细变形和Schauder不动点定理.     

Bifurcations of traveling wave solutions for the magma equation

The traveling wave solutions of the magma equation are studied by using the approach of dynamical systems and the theory of bifurcations. With the aid of Maple, all bifurcations and phase portraits in the parametric space are obtained. Under different regions of parametric space, various sufficient conditions to guarantee the existence of solitary wave, periodic wave and breaking wave solutions are given. Moreover, the reason for appearance of breaking waves is explained.     

Nonexistence results for a compressible non-Newtonian fluid with magnetic effects in the whole space

We consider a generalization of the compressible barotropic Navier-Stokes equations to the case of non-Newtonian fluid in the whole space. The viscosity tensor is assumed to be coercive with an exponent q>1. We prove that if the total mass and momentum of the system are conserved, then one can find a constant qγ>1 depending on the dimension of space n and the heat ratio γ such that for q∈[qγ,n) there exists no global in time smooth solution to the Cauchy problem. We prove also an analogous result for solutions to equations of magnetohydrodynamic non-Newtonian fluid in 3D space.     

再生核空间偏微分方程解析数值解

１．引言 偏微分方程的近似解法一直是数值计算的重要内容之一。随着计算机的发展,各种实用的新方法也不断涌现．本文在再生核空间Ｈ　（Ｄ）中给出二阶偏微分方程边值问题解析形式的级数解,该级数解具有如下特点：１．级数截断就可直接得到解析数值解;２．解析数值解的误差在空间范数意义下单调下降． 设 Ｄ＝［ａ, ｂ］ ｘ ［ｃ, ｄ］是 Ｒ２中的任一矩形域, Г为边界,０,ｕ（ｘ,ｙ）∈Ｌ２（Ｄ）且是实的绝对连续函数,中规定内积如下： 范数定义为： 山中已证明码（利是一个再生核函数空间,其再生校函数研Ｘ,认（,…表达式…     

A new method for solving singular fourth-order boundary value problems with mixed boundary conditions

In [1], [2], [3], [4], [5], [6], [7] and [8], it is very difficult to get reproducing kernel space of problem (1). This paper is concerned with a new algorithm for giving the analytical and approximate solutions of a class of fourth-order in the new reproducing kernel space. The numerical results are compared with both the exact solution and its n-order derived functions in the example. It is demonstrated that the new method is quite accurate and efficient for fourth-order problems.     

The exact solution of a linear integral equation with weakly singular kernel

A space , which is proved to be a reproducing kernel space with simple reproducing kernel, is defined. The expression of its reproducing kernel function is given. Subsequently, a class of linear Volterra integral equation (VIE) with weakly singular kernel is discussed in the new reproducing kernel space. The reproducing kernel method of linear operator equation Au=f, which request the image space of operator A is and operator A is bounded, is improved. Namely, the request for the image space is weakened to be L²[a,b], and the boundedness of operator A is also not required. As a result, the exact solution of the equation is obtained. The numerical experiments show the efficiency of our method.     

Blow Up of Classical Solutions to $\Box$ U=|u|1+α in Three Space Dimensions

We study the life span of classical solutions to ◻u = |u|^{1+α} in three space dimensions with initial data t = 0: u = εf(x), u, = εg(x), where f and g have compact support and are not both identically zero, ε is a small parameter. We obtain respectively upper and lower bounds of the same order of magnitude for the life span for sufficiently small ε in case 1 ≤ α ≤ \sqrt{2}. We also proved that the classical solution always blows up even when ε = 1 in the critical case α = \sqrt{2}.     

Traveling wave solutions for fractional partial differential equations arising in mathematical physics by an improved fractional Jacobi elliptic equation method

In this paper, combining with a new generalized ansätz and the fractional Jacobi elliptic equation, an improved fractional Jacobi elliptic equation method is proposed for seeking exact solutions of space‐time fractional partial differential equations. The fractional derivative used here is the modified Riemann‐Liouville derivative. For illustrating the validity of this method, we apply it to solve the space‐time fractional Fokas equation and the the space‐time fractional BBM equation. As a result, some new general exact solutions expressed in various forms including the solitary wave solutions, the periodic wave solutions, and Jacobi elliptic functions solutions for the two equations are found with the aid of mathematical software Maple. Copyright © 2016 John Wiley & Sons, Ltd.