时滞Liénard方程解的有界性

研究时滞Li啨nard方程¨x+f1(x)·x+f2(x(t-τ))·x(t-τ)+g(x(t-τ))=e(t)的解的有界性,其中f1,f2均连续可微,g(t)可微,e(t)为连续函数,当f2=0时,上方程就化为文献[9]中研究的方程¨x+f(x)·x+g(x(t-τ))=e(t).结果推广了文献[9]中的结论.     

一类具有两个偏差变元的高阶微分方程反周期解的存在唯一性

利用Leray-Schauder度理论,获得一类具有两个偏差变元的高阶微分方程x(n)(t)+f(t,x'(t),x'(t),…,x(n-1)(t))+g1(t,x(t-r1(t)))+g2(t,x(t-r2(t)))=e(t)反周期解存在唯一性的充分条件.     

一般次线性条件下脉冲方程的周期解

次线性条件下,脉冲系统x"+f(t,x)=0,a.e.t∈[0,2π]Δx'(t_j):=x'(t+j)-x'(t_j~-)=I_j(x(t_j))j=1,2,…,p的周期解的存在性被广泛研究.这里的次线性主要体现在f(t,x)被下面次线性函数控制:|f(t,x)|≤g(t)|x|α+h(t)其中g,h∈L~1(0,2π;R~+),α∈[0,1).本文减弱了上述次线性控制的要求,利用临界点理论证明了当f(t,x)满足某个函数类条件时,脉冲方程周期解是存在的,从而推广了相关结果.     

一类二阶非线性微分方程解的有界性和渐近稳定性

本文给出了方程 [(a(t)x′)′+h(t,x,x′)x′+q(t)f(x)g(x′)=e(t,x,x′)的解的有界性和渐近稳定性的充分条件,所得结果改进和包含了一些已知的结果。     

一类非线性泛函微分方程的振动性准则

给出了带强迫项的二阶非线性微分方程x″(t)+p(t)f(x(t),x(τ(t)))g(x′(t))=e(t)振动的若干新的充分条件,改进并推广了孙元功(2003)的结果.     

单侧条件下Liénard系统的调和解

研究了一类二阶微分方程x″+f(x)x′+g(x)=e(t)调和解的存在性.假设f(x)有界,g(X)满足新的单侧条件,即当x≥d时g(x)/x≥a,以及当x＜d时g(x)满足次线性条件或者有界,应用连续引理,得到了调和解的存在性定理.     

一类Liénard型方程周期解及概周期解的存在唯一性和渐近稳定性

应用 V-函数法讨论具有强迫项的 L iénard方程 x+f0 (x) x+f1 (x) x2 +g(x) =e(t)周期解与概周期解存在唯一性和渐近稳定性     

半狄氏型的符号光滑测度扰动

假设(Xt,Px)是与L2(E;m)上的半狄氏型((e),D((e)))相联系的右过程.μ为符号光滑测度,Aμt为μ对应的连续可加泛函.定义广义Feynman-Kac半群Pμtf(x)∶=Ex[e-tf(Xt)].设(e)μ(f,g)=(e)f,g)+(f,g)μ,(V)f,g∈D((e)μ)=D((e))∩L2(E,|μ|),我们得到以下两个命题等价:①((e)μ,D((e)μ))是下半有界的;②对任意的t＞0,存在一个常数α0≥0使得||Pμt|2≤eα0t.如果①和②中有一个成立,则(Pμt)t≥0是L2(E;m)上强连续的半群.     

具强迫项的二阶非线性泛函微分方程解的振动性与渐近性

建立一类具有强迫项的二阶非线性泛函微分方程[p(t,x(t)x'(t)]' f(t,x(t),x(g(t)),x'(t),x'(h(t)))=e(t)的振动准则，并讨论解的渐近性。     

具有强迫项的有限时滞Lienard方程周期解的存在性

利用Mawhin延拓定理证明,构造新算子,使用新技巧,研究了一类具有强迫项和有限时滞的二阶Lienard方程x″(t)+f1(x)x'(t)+f2(x)(x'(t))2+g(x(t-τ))=e(t)的周期解问题,得到了方程至少存在一个周期解的充分条件,获得了新的结论.     

Melnikov函数在含有两个幂零尖点的双异宿环附近的展开式

考虑未扰Liénard系统ẋ=y,ẏ=-g（x）,其中deg g（x）=7,当该系统分别含有2,3,4和5个奇点时,给出了其所有的不同拓扑类型的相图,并给出了Melnikov函数在含有2个幂零尖点和1个双曲鞍点的双异宿环附近的展开式和得到极限环的条件.     

n阶非线性泛函微分方程正解存在的几个充要条件

利用Ｓｃｈａｕｄｅｒ不动点定理讨论ｎ阶非线性泛函微分方程ｘ￣（ｎ）（ｔ）＋ｐ（ｔ）ｆ（ｘ（ｇ（ｔ）＝ｒ（ｔ）正解全体的构成与正解的存在性．     

Global and non-global solutions to some chemotaxis model

The paper is concerned with some chemotaxis model ∂u/∂t=D▿(u▿ln(u/w))+u(a−bu),∂w/∂t=f(u,w). To study the behavior of the solution, some function transformations are introduced, and the main tool is sup-sub-solution method. The result shows that, whether the solution blows up in finite time depends on the parameters and the initial data. As the chemical substance w has linear growth, f(u,w)=βu−δw, where β>0, δ>0 and a+δ>0, wherein the solution exists globally. However, as w possesses exponential growth, f(u,w)=(βu−δ)w, wherein both u and w share the same blowup point and time if the solution blows up in finite time. Biography: CHEN Hua(1956–), male, Professor, Ph. D., research direction: partial differential equation and its application.     

The Distribution of a CP-asymmetric quantity in the decay channel J / Ψ → π + π ? π 0

The distribution of a CP-asymmetric quantityA in the decay channelJ/ψ→π ⁺ π ⁻ π ⁰ is investigated. This dimensionless quantityA is constructed from the momenta of the π-meson final states, namely A=P _x ^{π +} P _y ^{π −} -P _x ^{π −} P _y ^{π −}, whereP _h,P _x ^h andP _y ^h are the module of the momentum of a hadron h, the x- and y-components of that momentum respectively, theJ/ψ particle is produced by e⁺ e⁻ collision, and the direction of the momentum of e⁺ is taken to be the positive direction ofz axis. There would exists the violation under the combined transformation of charge conjugation and space reflection (CP violation) when the average ofA among a lot of events, 〈A〉, be examined to be nonzero clearly from data. In this way, 748 events are selected from the BES experimental data, and analyzed. The corresponding averageA-value is measured to be 〈A〉 = 0.010 39 ± 0.014 61 ± 0.015 2. Further, some discussion of our result, the size of the data sample being need for further attempt and a possible perspective are given.     

New orthonormal and complete representation for complex scalar fields

The explicit common eigenvectors for complex scalar fields φ (x) and φ+ (x) are derived . They span an orthonormal and complete space. Based on this, the charge conjugate unitary operator and the operator which generates Bogolyubov pseudo-particles transformation can be neatly derived. It is emphasized that | ξ> is different from the direct product of two independent eigenvectors respectively belonging to two real scalar fields, and | ξ > is named the correlated eigenstates of φ( x) and φ+ (x).     

PCln (n=-1,0,+1)分子离子基态的结构与势能函数

 基于Gaussian03计算软件,选用高角动量基函数6-311++g(df,pd),分别使用密度泛函理论UB3LYP和UB3P86,以及组态相互作用方法UCCSD-FC和UQCISD-FC,对PCl分子和PCl⁺,PCl^-离子基态进行了几何优化,进一步对其进行了频率计算和单点能扫描计算.用最小二乘法拟合得到了PCl^<em>n(n=-1,0,+1)分子离子基态的Murrell-Sorbie势能函数.与实验及理论结果比较表明,对PCl,PCl⁺分子离子基态光谱常数 (B_e,α_e,ω_e,ω_ex_e)的计算结果达到了很高的精度.文章还首次给出PCl^-分子离子基态光谱参数(B_e,α_e,ω_e,ω_ex_e)和PClⁿ(n=-1,0,+1)力常数(f₂,f₃,f₄)的理论数据,为PClⁿ(n=-1,0,+1)分子离子的更深层次研究和应用提供重要的理论基础.     

Multi-parameter infinite-dimensional (r,δ)-OU process

The definition of n-parameter infinite-dimensional (r,δ) -Ornstein-Uhlenbeck process {xt (·) } ((r, δ)-OUPn∞ for short) is given. The absolute continuity of distribution μt of Xt(·) and the limit of Xt(·) when |t| →∞ is discussed.     

Nonlinear version of Holub’s theorem and its application

Holub proved that any bounded linear operator T or -T defined on Banach space L 1(μ) satisfies Daugavet equation1+‖T‖=Max{‖I+T‖, ‖I-T‖}.Holub's theorem is generalized to the nonlinear case: any nonlinear Lipschitz operator f defined on Banach space l 1 satisfies1+L(f)=Max{L(I+f), L(I-f)},where L(f) is the Lipschitz constant of f. The generalized Holub theorem has important applications in characterizing the invertibility of nonlinear operator.