具有细鞍点的二次系统

发散量为零的初等奇点,如果它是焦点,称它为细焦点;如果它是鞍点,称它为细鞍点。在二次系统的研究中。在某些场合,细鞍点与细焦点起到类似的作用。例如,具有两个细焦点(细鞍点)或一细焦点一细鞍点的二次系统必无极限环。若存在一个细焦点(细鞍点),则另外的细焦点至多是一阶的。本文进一步研究了具有细鞍点的二次系统,发现了与具有细焦点的二次系统有许多不同的性质。例如。具有细焦点的二次系统,其极限环未必集中分布,而本文证明:具有细鞍点的二次系统若存在极限环,则必集中分布(定理1)。我们还给出了点O外围存在极限环和不存在极     

一类四次系统极限环的个数与分布

本文研究一类四次系统的极限环,通过计算四次系统鞍点分界线之间的有向距离,计算一阶焦点量及二阶焦点量,判别同宿轨内外的稳定性,利用分支理论与定性分析技巧发现这类系统有六个极限环,并给出了它们的分布.     

二次系统极限环的相对位置与个数

<正> 中的P_2(x,y)与Q_2(x,y)为x,y的二次多项式.文[1].曾指出,系统(1)最多有三个指标为+1的奇点,且极限环只可能在两个指标为+1的奇点附近同时出现.如果方程(1)的极限环只可能分布在一个奇点外围,我们就说此系统的极限环是集中分布的.本文主要研究具非粗焦点的方程(1)的极限环的集中分布问题,和极限环的最多个数问题.文[2]-[5]曾证明,当方程(1)有非粗焦点与直线解或有两个非粗焦点或有非粗焦点与具特征根模相等的鞍点时。方程(1)无极限环.本文给出方程(1)具非粗焦点时,极限环集     

一类四次系统极限环的个数与分布

本文研究一类四次系统的极限环,通过计算四次系统鞍点分界线之间的有向距离,计算一阶焦点量 及二阶焦点量,判别同宿轨内外的稳定性,利用分支理论与定性分析技巧发现这类系统有六个极限环, 并给出了它们的分布．     

具有细链双曲无穷远鞍点的二次系统

本文得到：具有细链双曲无穷远鞍点和一个细焦点的二次系统至多存在一个极限环,若有细无穷远分界线环S,则其内部不存在极限环,其稳定性与它包围的奇点的稳定性相反．     

关于平面二次系统的极限环

本文对只有两个焦点和一个无限远鞍点的二次系统,用全局分析的方法得出极限环大范围存在的二组新型条件.在此基础上,联合Баутин,秦元勋扰动细焦点产生极限环的方法,在参数空间中找到一个十二维和一个十一维的流形,使对应的二次系统至少有四个极限环.顺便指出:Баутин算错了V₇的符号,它直接影响一个极限环的存在性.     

二次系统的细鞍点与分界线环

类似于扰动法,P.Joyal引进了细鞍点的鞍点量概念,并讨论了鞍点量与经过该鞍点的同宿轨道(即只经过一个鞍点的分界线环,记为S~((1))产生极限环的个数之间的关系.本文给出二次系统的鞍点量用系数表示的公式,为研究二次系统的分界线环在何种条件下能扰动出极限环及其个数提供了重要的工具.     

二次微分系统(III)_n=0的极限环和分支现象

本文应用分支理论得到了二次系统（ＩＩ）ｎ＝０在Ｏ（０，０）外围极限环的存在和数目及分界线环和半稳定环分支曲线的所有可能的分支图进一步地，证明了该系统在Ｏ外围至多有三个极限环，且有以一个有限和两个无穷远鞍点或鞍结点为顶点的非单值多边环     

关于平面二次系统的极限环

关于常微分方程二次系统的极限环及分布结构,本文得到下述定理: 设有一个三阶细焦点,并且无限远奇点是唯一的简单的奇点,则必存在另外一个粗焦点。在粗焦点外有奇数个极限环,无限远奇点为鞍点,全局结构已定。 在上述的基础上对方程作参数的微小变化,使三阶细焦点跳出三个极限环,则得二个粗焦点,每个外面有奇数个极限环,总极限环数为偶数个,并至少为4个,全局结构已定。     

分界线环的稳定性和分支极限环的唯一性

本文证明若在鞍点处发散量保持为零,则在分界线环L_0分支出极限环的过程中发散量积分是连续的,因而当发散量沿L_0的积分不为零时,L_0产生的极限环是唯一的。本文还证明,仅由细鞍点的阶数和鞍点量的符号并不能给出判定过细鞍点的单叶(双叶)同宿分界线环的内侧(内外侧)稳定性的普适准则。最后证明具有以细鞍点为重点的不可约三次代数曲线解的二次微分系统必可积;二次系统的同宿分界线环因改变稳定性而生成的极限环是唯一的。     

The planar discontinuous piecewise linear refracting systems have at most one limit cycle

In this paper we investigate the limit cycles of planar piecewise linear differential systems with two zones separated by a straight line. It is well known that when these systems are continuous they can exhibit at most one limit cycle, while when they are discontinuous the question about maximum number of limit cycles that they can exhibit is still open. For these last systems there are examples exhibiting three limit cycles.The aim of this paper is to study the number of limit cycles for a special kind of planar discontinuous piecewise linear differential systems with two zones separated by a straight line which are known as refracting systems. First we obtain the existence and uniqueness of limit cycles for refracting systems of focus-node type. Second we prove that refracting systems of focus–focus type have at most one limit cycle, thus we give a positive answer to a conjecture on the uniqueness of limit cycle stated by Freire, Ponce and Torres in Freire et al. (2013). These two results complete the proof that any refracting system has at most one limit cycle.     

A Note on the Bendixson-Dulac Theorem for Refracted Systems with Multiple Zones

This note extends the Bendixson-Dulac theorem to refracted systems with multiple zones. As an application, we prove that piecewise linear Duffing-type system has neither crossing limit cycles nor sliding limit cycles Therefore, it gives a positive answer to the Conjecture of \cite{TA2007}.     

Limit cycles of piecewise linear dynamical systems with three zones and lateral systems

In this paper, we give some evidences what cause more limit cycles for piecewise dynamical systems. We say, the angles or the number of zones are critical points. We study an example of linear lateral systems and an example of linear Y-shape systems, and prove that they have five and four crossing limit cycles by using Newton-Kantorovich Theorem, respectively.     

Limit cycles of discontinuous piecewise differential systems formed by linear centers in R2 and separated by two circles

We show that discontinuous planar piecewise differential systems formed by linear centers and separated by two concentric circles can have at most three limit cycles. Usually is a difficult problem to provide the exact upper bound that a class of differential systems can exhibit. Here we also provide examples of such systems with zero, one, two, or three limit cycles.     

Algebraic limit cycles of degree 4 for quadratic systems

Yablonskii (Differential Equations 2 (1996) 335) and Filipstov (Differential Equations 9 (1973) 983) proved the existence of two different families of algebraic limit cycles of degree 4 in the class of quadratic systems. It was an open problem to know if these two algebraic limit cycles where all the algebraic limit cycles of degree 4 for quadratic systems. Chavarriga (A new example of a quartic algebraic limit cycle for quadratic sytems, Universitat de Lleida, Preprint 1999) found a third family of this kind of algebraic limit cycles. Here, we prove that quadratic systems have exactly four different families of algebraic limit cycles. The proof provides new tools based on the index theory for algebraic solutions of polynomial vector fields.     

The number and stability of limit cycles for planar piecewise linear systems of node–saddle type

The objective of this paper is to study the number and stability of limit cycles for planar piecewise linear (PWL) systems of node–saddle type with two linear regions. Firstly, we give a thorough analysis of limit cycles for Liénard PWL systems of this type, proving one is the maximum number of limit cycles and obtaining necessary and sufficient conditions for the existence and stability of a unique limit cycle. These conditions can be easily verified directly according to the parameters in the systems, and play an important role in giving birth to two limit cycles for general PWL systems. In this step, the tool of a Bendixon-like theorem is successfully employed to derive the existence of a limit cycle. Secondly, making use of the results gained in the first step, we obtain parameter regions where the general PWL systems have at least one, at least two and no limit cycles respectively. In addition for the general PWL systems, some sufficient conditions are presented for the existence and stability of a unique one and exactly two limit cycles respectively. Finally, some numerical examples are given to illustrate the results and especially to show the existence and stability of two nested limit cycles.     

About the Sojourn Time Process in Multiphase Queueing Systems

Multiphase queueing systems (MQS) (tandem queues, queues in series) are of special interest both in theory and in practical applications (packet switch structures, cellular mobile networks, message switching systems, retransmission of video images, asembly lines, etc.). In this paper, we deal with approximations of MQS and present a heavy traffic limit theorems for the sojourn time of a customer in MQS. Functional limit theorems are proved for the customer sojourn time – an important probability characteristic of the queueing system under conditions of heavy traffic.      

CALCULATION OF FOCAL VALUES FOR E_3~1 SYSTEMS

1IlltroductionInthispaper)weconsiderthenumberoflimitcyclesforthefollowingcubicpolynomialdifferentialsystemForthepurposeofanalysingthenumberoflimitcycles,inawaylitisnecessarytocalculatethefocalvalues.Alotofworkonquadraticsystemshavebeendone.Now,manymathematicianshaveturntheirinteresttocubicsystems.However,itismoredifficultforacubicsystems,becausethealgorithmcomplicacyforcalculatingthefocalvalueisexponentiallyincreasing.Attemptoperformthecalculationbyhandisnotpossible.Someonehasstudiedsomespec…     

Highly nonlinear large-competition limits of elliptic systems

This article is concerned with the effect of different types of competitive interaction terms on the large-interaction limit of nonlinear elliptic systems modelling the steady states of populations that compete in some region. As the competition rate tends to infinity, we show that non-negative solutions of quite simple-looking systems converge to the positive and negative parts of a solution of a scalar limit problem which may be much more strongly nonlinear than the original system, possibly with quadratic growth in the gradient of the limit function.     

Integrable Systems Obtained by Puncture Fusion from Rational and Elliptic Gaudin Systems

Using the procedure for puncture fusion, we obtain new integrable systems with poles of orders higher than one in the Lax operator matrix and consider the Hamiltonians, symplectic structure, and symmetries of these systems. Using the Inozemtsev limit procedure, we find a Toda-like system in the elliptic case having nontrivial commutation relations between the phase-space variables.