区间上单峰扩张自映射周期轨道的超旋转对

设f是区间I=[0,1]上的单峰扩张自映射,k∈N,m≥2,λm,k是方程x(k-1)m(xm-1)Q(x,m+1)+(x(k-1)m-1)Q(x,m)=0在(1,+∞)上的唯一实根,其中Q(x,m)=(xm-2xm-1+1).本文证明若f的扩张常数λ≥λm,k,则f有超旋转对为(k,km+1)的周期轨道.此外,还指出,当1＜λ＜λm,k时,在区间上存在单峰扩张自映射具有扩张常数λ却无超旋转对为(k,km+1)的周期轨道.     

区间上单峰扩张自映射周期轨道的超旋转对

设f是区间I=[0,1]上的单峰扩张自映射, k ∈N,m≥2,λm,k是方程x(k-1)m(xm- 1)Q(x,m 1) (x(k-1)m-1)Q(x,m)=0在(1, ∞)上的唯一实根,其中Q(x,m)=(xm- 2xm-1 1).本文证明:若f的扩张常数λ≥λm,k,则f有超旋转对为(k,km 1)的周期轨道. 此外,还指出,当1<λ<λm,k时,在区间上存在单峰扩张自映射具有扩张常数λ却无超旋转对为(k,km 1)的周期轨道.     

区间上平顶单峰扩张自映射的周期轨道

设ｔ（０＜ｔ＜１）是一个常数，ｎ≥３是奇数，ｍ≥０及ｋ≥１是整数，Ｐ０（ｘ）＝ｘ－１，Ｐｉ（ｘ）＝（ｘ２ｉ－１－１）Ｐｉ－１（ｘ）（ｉ≥１），ｒｍｎ（ｔ）及ｒｋ（ｔ）分别是方程Ｐｍ（ｘ）（ｘ２ｍｎ－２ｘ２ｍ（ｎ－２）－１）－ｔ（ｘ２ｍｎ－１）（ｘ２ｍ＋１）＝０及Ｐｋ－１（ｘ）－ｔ（ｘ２ｋ－１＋１）＝０在（１，＋∞）上的唯一实根，ｆ是闭区间Ｉ＝［０，１］上的峰顶区间长度为ｔ的平顶单峰扩张自映射．本文证明了，若ｆ的扩张常数λ≥ｒｍｎ（ｔ）（或＞ｒｋ（ｔ）），，则ｆ有２ｍｎ（或２ｋ）周期点．此外，本文还指出，当１＜λ＜ｒｍｎ（ｔ）（或≤ｒｋ（ｔ）时，在Ｉ上存在着具有扩张常数λ及峰顶区间长度ｔ却无２ｍｎ（或２ｋ）周期点的平顶单峰扩张自映射     

关于区间上的单峰扩张自映射

设ｆ是区间Ｉ＝［０，１］上的扩张的单峰函数，λ是ｆ的扩张常数。又设Ｋ≥３是奇数，ｎ≥３是整数，λｋ是方程ｘ＾ｋ－２ｘ＾ｋ－２－１＝０的最大实根，μｎ是方程ｘ＾ｎ－２ｘ＾ｎ－１＋１＝０的最大实根，本文用较简单的方法证明了，当λ≥λＫ时，ｆ中含有Ｋ－周期轨道，当λ≥μｎ时，ｆ中含有相对于自身的ＲＬ＾ｎ－２Ｃ型单峰周期轨道。此外，本文还讨论了一类方程ｘ＾ｎη（ｘ）＝ζ（ｘ）的根的极限度最性质。     

区间上k段单调连续自映射的k阶迭代根

本文得到了区间Ｉ＝［０，１］上的ｋ段单调连续自映射具有ｋ阶迭代根的充要条件     

关于一类自映射轨道的研究

1 概念及已有结果 设X为拓扑空间,f∈C0（X,X）,f0表示恒等映射,对任意自然数n,定义fn=fοfn-1. 称O（x,f）={fn（x）│n=0,1,2,… ;x∈X}为x的f轨道. 关于周期点、周期点集、周期、周期轨道,Sarkovskii序如通常定义,可参见[1].     

区间上满的扩张Markov自映射的迭代根

考虑区间上满的扩张 Markov自映射 ,给出了区间上满的扩张 Markov自映射具有指定阶的迭代根的充分必要条件 .     

流形上广义扩张自映射

本文将紧流形上的扩张自映射推广到广义的扩张自映射.一方面,广义扩张自映射的一系列动态性质与扩张自映射的表现类似,参考文 M.Shub[3],并且任何扩张自映射在一定的 Riemann 度量下均可成为广义扩张自映射.另一方面,在这两类自映射之间存在着一个重要的差别,这就是扩张自映射是结构稳定的,而广义扩张自映射可以不是.本文所有的术语均可在文 S.Smale[4]中找到.     

环的自映射的最少周期点数

设Ｘ是一个紧致连通的ＡＮＲ＇ｓ，ｆ：Ｘ→Ｘ是连续映射。于是ｆ有Ｎｉｅｌｓｅｎ型数，ＮＦｎ（ｆ），它是数集｛＃Ｆｉｘ（ｇ＾ｎ）ｇ－ｆ｝的下界。本文在Ｘ是环时，给出ＮＦｎ（ｆ）是该数集的下确界，即存在连续映射ｇ＝ｆ，使得＃Ｆｉｘ（ｇ＾ｎ）＝ＮＦｎ（ｆ）的一个充分条件。     

区间上一类连续自映射的单调迭代根

设Ｉ＝［０,１］,０＜ａ＜ｂ＜１,记Φ_ab≡｛Ｆ∈Ｃ^０（Ｉ）：Ｆ｜［０,ａ］和Ｆ｜［ｂ,１］严格单调递增且Ｆ在［ａ,ｂ］恒取常值｝．本文讨论了Ｆ∈Φ_ab有单调迭代根的充要条件．     

Numerical Continuation of Hamiltonian Relative Periodic Orbits

The bifurcation theory and numerics of periodic orbits of general dynamical systems is well developed, and in recent years, there has been rapid progress in the development of a bifurcation theory for dynamical systems with structure, such as symmetry or symplecticity. But as yet, there are few results on the numerical computation of those bifurcations. The methods we present in this paper are a first step toward a systematic numerical analysis of generic bifurcations of Hamiltonian symmetric periodic orbits and relative periodic orbits (RPOs). First, we show how to numerically exploit spatio-temporal symmetries of Hamiltonian periodic orbits. Then we describe a general method for the numerical computation of RPOs persisting from periodic orbits in a symmetry breaking bifurcation. Finally, we present an algorithm for the numerical continuation of non-degenerate Hamiltonian relative periodic orbits with regular drift-momentum pair. Our path following algorithm is based on a multiple shooting algorithm for the numerical computation of periodic orbits via an adaptive Poincaré section and a tangential continuation method with implicit reparametrization. We apply our methods to continue the famous figure eight choreography of the three-body system. We find a relative period doubling bifurcation of the planar rotating eight family and compute the rotating choreographies bifurcating from it.      

具有给定能量的引力势N体型问题的多个闭轨

本文对一类Ｎ体型Ｈａｍｉｌｔｏｎ系统证明了在任一给定能量面上存在多个几何不同的非碰撞周期轨道．     

The Centres of Gravity of Periodic Orbits

Let $f : I → I$ be a continuous map. If $P(n, f) = \{x ∈ I; f^n (x) = x \}$ is a finite set for each $n ∈\boldsymbol{N}$, then there exists an anticentered map topologically conjugate to $f$, which partially answers a question of Kolyada and Snoha. Specially, there exists an anticentered map topologically conjugate to the standard tent map.     

Bifurcations of Periodic Points of Holomorphic Maps From C2 into C2

Let F:Cⁿ Cⁿ be a holomorphic map, F^k be the kth iterate ofF, and p Cⁿ be a periodic point of F of period k. That is,F^k(p) = p, but for any positive integer j with j < k, F^j(p) p. If p is hyperbolic, namely if DF^k(p) has no eigenvalue ofmodulus 1, then it is well known that the dynamical behaviourof F is stable near the periodic orbit = {p, F(p),..., F^k–1(p)}.But if is not hyperbolic, the dynamical behaviour of F near may be very complicated and unstable. In this case, a veryinteresting bifurcational phenomenon may occur even though may be the only periodic orbit in some neighbourhood of : forgiven M N\{1}, there may exist a C^r-arc {F_t: t [0,1]} (wherer N or r = ) in the space H(Cⁿ) of holomorphic maps from Cⁿinto Cⁿ, such that F₀ = F and, for t (0,1], F_t has an Mk-periodicorbit _t with as t 0. Theperiod thus increases by a factor M under a C^r-small perturbation!If such an F_t does exist, then , as well as p, is said to beM-tupling bifurcational. This definition is independent of r. For the above F, there may exist a C^r-arc in H(Cⁿ), with t [0,1], such that and, for t (0,1], has two distinct k-periodic orbits _t,1 and _t,2 with d(_t,i, ) 0 as t 0 for i = 1,2. If such an does exist, then , as well as p, is said to be 1-tupling bifurcational. In recent decades, there have been many papers and remarkableresults which deal with period doubling bifurcations of periodicorbits of parametrized maps. L. Block and D. Hart pointed outthat period M-tupling bifurcations cannot occur for M >2 in the 1-dimensional case. There are examples showing thatfor any M N, period M-tupling bifurcations can occur in higher-dimensionalcases. An M-tupling bifurcational periodic orbit as defined here actsas a critical orbit which leads to period M-tupling bifurcationsin some parametrized maps. The main result of this paper isthe following. Theorem. Let k N and M N, and let F: C² C² be a holomorphicmap with k-periodic point p. Then p is M-tupling bifurcationalif and only if DF^k(p) has a non-zero periodic point of periodM. 1991 Mathematics Subject Classification: 32H50, 58F14.     

寻找周期轨道的代数分析法

本文给出了计算一般代数型（有理分式）离散动力系统周期轨道的一种分析方法－代数分析法。这种方法的优点是将非线性求解问题转化为一个线性求解问题来处理。它不仅可以准确地确定包括稳定和不稳定周期轨道的位置，而且还可以详细了解周期轨道的产生和随参数演变的分岔特性。本文利用这种方法分析了一个四维二次非线性映射，并给出了其完整的低周期轨道的分岔曲线图。     

非线性空间上的大范围周期轨道之同调类

非线性力学系统的大范围周期轨道可以代表等能曲面上的同调类,这些同调类一般非平凡,而等能曲面的拓扑性质又由相空间的拓扑性质及哈密顿函数的大尺度性质决定。本文用后两类性质估算了等能曲面的第1同调群的秩。     

一类二阶渐近周期Hamilton系统同宿轨道

运用变分方法讨论二阶渐近周期Hamilton系统 -u+L(t)u=(1+g(t))V′(t,u)的Lagrange泛函在流形上的极小问题,进而证明该系统存在非平凡同宿轨道,其中L,V关于t是周期的,g(t)→0(|t|→∞).     

NMS Flows on Three-Dimensional Manifolds with One Saddle Periodic Orbit

The simplest NMS flow is a polar flow formed by an attractive periodic orbit and a repulsive periodic orbit as limit sets.In this paper we show that the only orientable,simple,compact,3-dimensional manifolds without boundary that admit an NMS flow with none or one saddle periodic orbit are lens spaces. We also see that when a fattened round handle is a connected sum of tori, the corresponding flow is also a trivial connected sum of flows.