连结奇点的轨线

本文利用孤立块和动力系统中典型区域的工具,给出了存在连结微分方程的两个奇点的轨线的几个充要条件,揭示了连结奇点的轨线与闭轨线、奇异闭轨线及分界线的关系。     

连结奇点轨线的存在性

本文给出了判定平面动力系统两个奇点的连结轨线存在性的一个准则。     

孤立块与连结轨线的存在性

用孤立块的概念,给出了连结平面动力系统2个奇点的轨线的存在性准则。     

连结奇点的轨线

假定对平面的C~1向量场V,存在一个有界的连通区域B使得B上无奇点,且B的所有外出点都是严格的外出点。假定在B中恰有两个奇点O_1和O_2,其中O_1是完全不稳定的。假定在B中不存在只围绕O_1的闭轨线和奇异闭轨线。于是必存在位于B中的轨线连结O_1和O_2。     

一类平面微分系统极限环的存在性与唯一性

本文研究了平面微分系统ｘ＝－ｙ＋δｘ＋ｍｘｙ＋ａｙ２＋ｂｙ３，ｙ＝Ｆ（ｘ）的极限环的存在唯一性，比较完整地讨论了参数空间，在全平面得到了无环和环存在的参数区域，发展了文［１］提出的比较对称轨线的方法，证明了只含一个奇点的极限环的唯一性，同时指出了含三个奇点的闭轨线族和奇闻轨线的存在性．     

环面上具有有限个奇点的连续流的轨线的拓扑结构

<正> 环面上具有一个奇点的微分方程(连续流)的轨线的拓扑结构已解决.内容是:1.如有不可缩的周期轨线或奇闭轨线,则沿作为分界线的这种轨线将环面切开,成为若干个带域、圆环域和螺旋域,而且可以列举出来.2.如果没有不可缩的周期轨线或奇闭轨线,则必有非平凡的 P~+和 P~-稳定轨线.这时它是诸态备经型或奇异型适当改造而成(加上一个奇点以及可能的一朵花,还可能加上最多二个一端为奇点的带域).     

一类带有三次项的平面五次微分系统的全局拓扑结构分析

一类带有三次项的平面五次微分系统在Poincare变换下可以讨论系统的无穷远奇点的性质,进而得到奇点附近轨线的拓扑结构,并利用判断函数给出极限环存在与否的条件,补充完善了五次系统的定性分析.     

层焰系统奇点结构的研究

在一定的假设条件下,将气体燃烧的物理模型简化为层焰系统．借助于热力学理论和相关的守恒定律建立了层焰系统的数学模型并对其进行了深入地分析．利用常微分方程的定性理论和方法,结合燃烧的实际需要,对应于参数的不同取值,研究了位于瑞利线上奇点的个数和位置,确定了暴燃区和爆炸区内不同奇点的定性结构及其稳定性,给出了在反应速度-滞止焓平面及燃烧速度-滞止焓平面内层焰系统轨线的相图．     

半线性抛物型方程定义的光滑强单调流收敛于半渐近稳定的奇点

本文研究半线性抛物型方程定义的光滑强单调流的渐近性态，我们给出了具有有界轨线且不收敛于半渐近稳定奇点的点集在Ｘ￣α中是第一范畴的充要条件，我们还研究了全有序奇点弧的存在性和非平凡不变函数的存在性之间的等价关系。     

R~n中具有非双曲奇点的异宿分支

考虑具有两个非双曲奇点的n维异宿系统。对这类Rⁿ中的高余维分支问题,求得Melnikov型向量分支函数,以保证在两个非双曲奇点所分裂出的新奇点间存在异宿轨线。     

Orbits connecting singular points in the plane

This paper concerns the global structure of planar systems. It is shown that if a positively bounded system with two singular points has no closed orbits, the set of all bounded solutions is compact and simply connected. Also it is shown that for such a system the existence of connecting orbits is tightly related to the behavior of homoclinic orbits. A necessary and sufficient condition for the existence of connecting orbits is given. The number of connecting orbits is also discussed.Supported by the National Science Foundation of China Grant No. 10461003.     

Global structure for a class of dynamical systems

In this paper, we shall consider the global structure of positive bounded systems on the plane which have m singular points, but not any closed orbits and singular closed orbits. We shall prove that these systems have at least m−1 connecting orbits; and all the connecting orbits, homoclinic orbits and singular points constitute a compact simply connected set. Each of other orbits tends to a singular point as t→+∞, and approaches to the infinity as t→−∞.     

A topological degree for orbits connecting critical points of autonomous systems

An argument based on topological degree is used to obtain an existence theorem for orbits connecting two critical points of an autonomous system. The result is applied to the existence of viscous profiles approximating shock waves in weak solutions of systems of nonlinear conservation laws. A result for the case where the Morse indices of the two critical points differ by more than one is also obtained.     

Minimal orbits close to periodic frequencies

Let with h analytic of small norm. The problem of Arnold's diffusion consists in finding conditions on h which guarantee the existence of orbits Q of with connecting two arbitrary points of frequency space. Recently, J. N. Mather has found a sufficient condition for Arnold's diffusion; this condition is not read on h itself, but on the set of all action-minimizing orbits of . In this paper we try to characterize those action-minimizing orbits whose mean frequency is close to periodic. Received: November 26, 1996     

Multiple solutions for indefinite functionals and applications to asymptotically linear problems

In this paper, by means of Morse theory of isolated critical points (orbits) we study further the critical points theory of asymptotically quadratic functionals and give some results concerning the existence of multiple critical points (orbits) which generalize a series of previous results due to Amann, Conley, Zehnder and K.C. Chang. As applications, the existence of multiple periodic solutions for asymptotically linear Hamiltonian systems is investigated. And our results generalize some recent ones due to Coti-Zelati, J.Q.Liu, S.Li, etc.This research was supported in part by the National Postdoctoral Science Fund.     

A Genealogy of Convex Solids Via Local and Global Bifurcations of Gradient Vector Fields

Three-dimensional convex bodies can be classified in terms of the number and stability types of critical points on which they can balance at rest on a horizontal plane. For typical bodies, these are non-degenerate maxima, minima, and saddle points, the numbers of which provide a primary classification. Secondary and tertiary classifications use graphs to describe orbits connecting these critical points in the gradient vector field associated with each body. In previous work, it was shown that these classifications are complete in that no class is empty. Here, we construct 1- and 2-parameter families of convex bodies connecting members of adjacent primary and secondary classes and show that transitions between them can be realized by codimension 1 saddle-node and saddle–saddle (heteroclinic) bifurcations in the gradient vector fields. Our results indicate that all combinatorially possible transitions can be realized in physical shape evolution processes, e.g., by abrasion of sedimentary particles.     

Point-to-Periodic and Periodic-to-Periodic Connections

In this work we consider computing and continuing connecting orbits in parameter dependent dynamical systems. We give details of algorithms for computing connections between equilibria and periodic orbits, and between periodic orbits. The theoretical foundation for these techniques is given by the seminal work of Beyn in 1994, “On well-posed problems for connecting orbits in dynamical systems”, where a numerical technique is also proposed. Our algorithms consist of splitting the computation of the connection from that of the periodic orbit(s). To set up appropriate boundary conditions, we follow the algorithmic approach used by Demmel, Dieci, and Friedman, for the case of connecting orbits between equilibria, and we construct and exploit the smooth block Schur decomposition of the monodromy matrices associated to the periodic orbits. Numerical examples illustrate the performance of the algorithms. This revised version was published online in July 2006 with corrections to the Cover Date.     

Periodic solution and global structure of Oregonator

In this paper, we studied the periodic solution, connecting orbits between singular points and global structure in Oregonator.     

Bifurcation of critical points for continuous families of C 2 functionals of Fredholm type

Given a continuous family of C ² functionals of Fredholm type, we show that the nonvanishing of the spectral flow for the family of Hessians along a known (trivial) branch of critical points not only entails bifurcation of nontrivial critical points but also allows to estimate the number of bifurcation points along the branch. We use this result for several parameter bifurcation, estimating the number of connected components of the complement of the set of bifurcation points in the parameter space and apply our results to bifurcation of periodic orbits of Hamiltonian systems. By means of a comparison principle for the spectral flow, we obtain lower bounds for the number of bifurcation points of periodic orbits on a given interval in terms of the coefficients of the linearization.     

The Closed Orbits of a Class of Cubic Vector Fields in R3

In this paper, we investigate the isolated closed orbits of two types of cubic vector fields in R₃ by using the idea of central projection transformation, which sets up a bridge connecting the vector field X(x) in R₃ with the planar vector fields. We have proved that the cubic vector field in R₃ can have two isolated closed orbits or one closed orbit on the invariant cone. As an application of this result, we have shown that a class of 3-dimensional cubic system has at least 10 isolated closed orbits located on 5 invariant cones, and another type of 3-dimensional cubic system has at least 26 isolated closed orbits located on 13 invariant cones or 26 invariant cones.