一类高维时滞微分方程的周期解

本文考虑高维时滞微分方程ｘ′（ｔ）＝Ａ（ｔ,ｘ（ｔ））ｘ（ｔ）＋ｆ（ｔ,ｘ（ｔ－ｒ（ｔ）））其中（ｔ,ｘ）∈Ｒ^ｎ,Ａ（ｔ,ｘ）是ｎ×ｎ连续矩阵,ｆ（ｔ,ｘ）是ｎ维连续向量,ｒ（ｔ）是时间依赖的滞量,应用不动点定理,在确定的条件下,证明了该系统的周期解的存在性与唯一性     

指数型二分性和周期系统的周期解

先讨论指数型二分性成立的条件，在某种意义下推广了Ｌａｚｅｒ关于二分性的结果，之后，我们用该结论探讨Ｌａｓｏｔａ－Ｏｐｉｕｌ方程及方程ｘ＝ｆ（ｔ，ｘ），ｆ（ｔ＋ｗ，ｘ）＝ｆ（ｔ，ｘ），ｆ（ｔ，ｘ）∈Ｃ’（Ｒ＊Ｒ＾ｎ，Ｒ＾ｎ）的周期解的存在性，推广了文「２」的主要结果，并得到一些新的结果。     

强迫振动中周期解的存在性

本文主要研究了强迫振动方程：ｘ＋（ｆ（ｘ）＋ｇ（ｘ）ｘ）Ｘ＋ｈ（ｘ）＝ｅ（ｔ）的解的有界性以及周期解的存在性,这里ｆ（ｘ）,ｇ（ｘ）,ｈ（ｘ）在（－∞,＋∞）中连续,ｅ（ｔ）在「０,＋∞）上连续,得到了解的有界性与存在周期解的条件。     

函数f（x）＝｜sinβx／sinαx｜（α，β＞0）的周期性

函数ｆ（ｘ）＝｜ｓｉｎβｘ／ｓｉｎαｘ｜（α，β＞０）的周期性曾丕刚陕西省镇安县中学７１１５００定理函数ｆ（ｘ）：为周期函数的充要条件是为周期函数，Ｌ为周期．（２）若ｆ（Ｘ）是周期函数，设ｔ（ｔ＞０）是它的周期，则ｆ（ｘ＋ｔ）＝ｆ（Ｘ），即在定义域内...     

一类微分差分方程的周期解

本文研究微分差分方程ｘ＇（ｔ）＝－ｆ（ｘ（ｔ），ｘ（ｔ－τ１））－ｆ（ｘ（ｔ），ｘ（ｔ－τ２））－．．．－ｆ（ｘ（ｔ），ｘ（ｔ－τｎ））非平凡周期解的存在性问题，得到了一些判别准则，推广和改进了文［１－４］的工作。     

某些环的变换性条件

设Ｚ（Ｒ）是环Ｒ的中心，本文证明了下列的结果：（１）若Ｒ是一个Ｋｏｔｈｅ半单纯环，且对任意ａ，ｂ属于Ｒ，都存在一自然数Ｋ＝Ｋ（ａ，ｂ），一含有Ｘ＾２ｔ ｎ＝ｎ（ａ，ｂ）个Ｙ的字ｆＸ（Ｘ，Ｙ）及一整系数多项多式ψＸ（ｘ，ｙ）使得ａｂ＾ｋ－ｆＸ（ａ，ｂ）．ψＸ＇（ａ，ｂ）属于Ｚ（Ｒ）则Ｒ是交换环；（２）若Ｒ是一个Ｂａｅｒ半单纯环，对任意的ａ，ｂ属于Ｒ，都存在一自然Ｋ＝Ｋ（ａ，ｂ）≤１，一含有Ｘ＾２和ｎ     

关于两处错误的剖析与纠正

本刊１９９７年第３期《利用一次函数的保号性解题》一文给出，一次函数ｆ（ｘ）＝ｋｘ＋ｂ具有如下一条性质（Ａ≥０）：如果｜ｆ（ｍ）｜＞Ａ，｜ｆ（ｎ）｜＞Ａ，则ｘ∈［ｍ，ｎ］时，有｜ｆ（ｘ）｜＞Ａ．我们指出，这一结论是错误的．例如，取ｆ（ｘ）＝ｘ，有｜ｆ（...     

一类沿曲面的奇异积分算子的（L^∞,BMO）—有界性

设ｎ≥３，定义Ｔｆ（ｘ，ｘｎ）＝Ｐ．Ｖ．∫Ｒ＾ｎ－１ｂ（ｔ）Ｋ（ｔ）ｆ（ｘ＝ｔ，ｘｎ－Г（│ｔ│））ｄｔ，其中ｘ∈Ｒ＾ｎ－１，ｂ（ｔ）为Ｒ＾ｎ－１上的有界函数，Ｋ（ｔ）为Ｒ＾ｎ－１上满足Ｈｏｒｍａｎｄｅｒ条件的函数，且Г（ｓ）为〔０，∞）上的任意函数。本文给出了Ｔ为（Ｌ∞（Ｒ＾ｎ），ＢＭＯ（Ｒ＾ｎ））一型，或等价地（Ｈ＾１（Ｒ＾ｎ），Ｌ＾１（Ｒ＾ｎ））一型时，ｂ所应满足的充分必要条件。     

最佳L2局部逼近存在唯一的充分必要条件

本文给出了最佳Ｌ２局部逼近的存在唯一性定理，设ｆ∈Ｌ２（０，δ），Ｓｎ＝ｓｐａｎ（ｕ０，ｕ１，．．．Ｕｎ－１）Ｃ＾ｎ－１（０，δ），且ｄｅｔＷｎ（ｕ０，ｕ１，．．．ｕｎ－１；０）≠０，那么，当ｘ→０时，网（Ｐｘ（ｆ，Ｓｎ）收敛于Ｓｎ中某元素Ｐ０（ｆ，Ｓｎ）的充要条件为：ｆ＝Ｐｎ－１＋ｈ，其中Ｐｎ－１（ｔ）＝ｎ－１∑ｉ＝１ａｉｔｉ（ｈ，１）ｘ＝０（Ｘ＾ｎ），ｘ→０，且Ｐ０（ｆ，Ｓｎ）＝ＵＷ＾－１ｎＡ     

相依样本下密度函数及其导函数的相合随机窗宽核估计

设（Ｘｎ）是Ｒ＾１中的平稳，强混合序列，具有公共的密度ｆ（ｘ），则可定义ｆ（ｘ）及其导函数ｆ＾（ｒ）（ｘ）的核估计与最近邻估计ｆ＾（ｒ）ｎ（ｘ）＝（ｎｈ＾ｒ＋１ｎ（ｘ））＾－１ｎ∑ｉ＝１Ｋ＾（ｒ）（Ｘｉ－Ｘ／ｈｎ（ｘ）），ｆｎ（ｘ）＝（ｎａｎ（ｘ））＾－１ｎ∑ｉ＝１Ｋ（Ｘｉ－ｘ／ａｎ（ｘ））其中核函数Ｋ（Ｘ）为取定的概率密度函数，且具有ｒ（ｒ≥０）阶导数，窗宽ｈｎ（ｘ）＝ｈｎ（ｘ；Ｘ１，．．．，Ｘ     

Maximal inequalities for a continuous semimartingale

Let X =( X t ) t S 0 be a continuous semimartingale given by d X t = f ( t ) w ( X t )d d M ¢ t + f ( t ) σ ( X t )d M t , X 0 =0, where M =( M t , F t ) t S 0 is a continuous local martingale starting at zero with quadratic variation d M ¢ and f ( t ) is a positive, bounded continuous function on [0, X ), and w , σ both are continuous on R and σ ( x )>0 if x p 0. Denote X 𝜏 * =sup 0 h t h 𝜏 | X t | and J t = Z 0 t f ( s ) } ( X s )d d M ¢ s ( t S 0) for a nonnegative continuous function } . If w ( x ) h 0 ( x S 0) and K 1 | x | n σ 2 ( x ) h | w ( x )| h K 2 | x | n σ 2 ( x ) ( x ] R , n >0) with two fixed constants K 2 S K 1 >0, then under suitable conditions for } we show that the maximal inequalities c p , n log 1 n +1 (1+ J 𝜏 ) p h Á X 𝜏 * Á p h C p , n log 1 n +1 (1+ J 𝜏 ) p (0< p < n +1) hold for all stopping times 𝜏 .     

approximation for the solutions of stochastic differential equations. iii. jointly weak convergence

We give sufficient conditions for a family Z, e > 0 of continuous finite variation processes to converge weakly to a diffusion process Z. Then we consider the integral equation dXE(t) = (l)(Xe(t))dZE{t) and the stochastic equation dX{i) = (j)(X{t))dZ{t) and denote by X(t,x,w respectively X{t,x,(jo), the solution starting at x. We prove that PoX~l, e>0 converge weakly to Pol     

OCCUPATION TIMES OF BALLS BY BROWNIAN MOTION WITH DRIFT

51. Introduction and Statement of ResultsLet X ~ {Xt, t 2 0} be a standajrd d-dimensional Brownian motion with drift c startedat fiXed XO ~ x:Xo ~ Wb ct, t 2 0,where Wt is the standard d--dimensional Brownian motion, c E R'(d 2 2) is a fixed vector.Denote by P:(.) the probability meajsure on the path space of X corresponding to initialstate XO = x and drift vector c, with E;(.) the corresponding expection operator. Forsimplity, we shall write Pz(.) and Ex(.) to refer to the case c ~ …     

Lienard方程周期解、概周期解的存在性

本文考虑Ｌｉｅｎａｒｄ方程ｘ”十ｆ（ｘ）ｘ’＋ｇ（ｘ）＝ｅ（ｔ），我们得到：当且时，对于任意周期或概周期。数ｅ（ｔ），它有周期或概周期解．而对于Ｌｉｅｎａｒｄ方程ｘ”＋ｆ（ｘ）ｘ’＋ｃｘ＝ｅ（ｔ），我们得到：当ｃ＞０且时，对于任意周期、或概周期函数ｅ（ｔ），它有周期或概周期解．     

条件经验随机过程的渐近性质

设(Xi,Yi)(i=1,2,…,n)是来自总体(X,Y)的样本(独立同分布),其中X∈R1,Y∈Rq.M(x y)是Y=y时X的条件分布,Mnkn(x y)为M(x y)的第kn个最近邻域的经验分布估计量,讨论条件经验过程Sn(t,x,y)=kn12(Mnkn(x y)-M(x y))的渐近性质,得出在适当条件下,对固定的y,Sn(t,x,y)(x,t为参数)弱收敛于某一G aussian过程S(.).     

Asymptotic equilibrium of ordinary differential systems

A theorem on asymptotic equilibrium is proved for the solutions of the system(1)X ⁿ=f(t,X), x ^t ₀=x_o where f(t,x) is majorized by a funciton g(t,u) which is non-increasing in u. It is of interest to notice that the funcitons f(t,x) and g(t,u) need not be defined for x=0 and u=0 respectively. Such majorant functions occur in gravitational problems and therefore the result is of pracitcal interest.Using this, the asymptotic relatiohship between the solutions of(2)y=A(t)y, y ^t _o=y_oand its nonlinear perturbation(3) X=A(t)x+f(t,x), X^t _o is investigated. This last result includes as a special case two theorems of Hallam[2]     

John and Uniform Domains in Generalized Siegel Boundaries

Potential Analysis - Given the pair of vector fields X = ?x + |z|2my?t and Y = ?y ?|z|2mx?t,where (x,y,t) = , we give a condition on a bounded domain which ensures...     

Nonlinear perturbation of linear evolution equations in a banach space

Summary Let X be a Banach space and {A(t)|t ε [0, T]} a family of closed linear, densely defined m-accretive operators in X. This paper is concerned with the additive perturbation of {A(t)|t ε [0, T]} by a continuous family of nonlinear accretive operators {B(t)|t ε [0, T]}. Namely solutions are provided for the integral equation u(t, τ, x) = W(t, τ)x − W(t, s)B(s) · · u(s, τ, x)ds, u(τ, τ, x) = x where W(t, s) is the linear evolution operator associated with the linear differential equation v'(t, s, x) + A(t)v(t, s, x) = 0, v(s, s, x) = x. Entrata in Redazione il 30 luglio 1975.     

STABILITY AND EXISTENCE OF PERIODIC SOLUTIONS AND ALMOST PERIODIC SOLUTIONS ON LIENARD SYSTEMS

1MainResultsConsidersystem11~.x f(x)x' g(x)~0(1)wheref(x)islocallyintegrable,g(x)isdifferentiablealldg(0)=0.Theroem1Thezerosolutionofsystem(1)isuniformlyasymptoticallystableifbyequivalenttransf'Ormu=xov=X' F(x).DefineW[t,(uif\v)]j6ug(s)ds Iv',thenwisaposi…     

Brown运动的逗留时与首中时

设为中的标准Brown运动,对0＜α,记本文求出了X在首中球面之前逗留在Bα内的时间的Laplace变换,在首中之前逗留在Bαb内的时间的Laplace变换以及在首中之前逗留在Bαb内的时间的Laplace变换．作为推论,求出了X关于球面首中时的Laplace变换,逗留在球内总的时间的Laplace变换及逗留在球壳内的总的时间的LaPlace变换．