Quadratic systems with a weak focus and a strong focus

It is proved that the quadratic system with a weak focus and a strong focus has a unique limit cycle around one of the two foci, if there exists simultaneously limit cycles around each of the two foci for the system.     

QUADRATIC SYSTEMS WITH A 3RD-ORDER (OR 2ND-ORDER) WEAK FOCUS

1 IntroductionSince a quadratic system has no limit cycle around a 3rd-order weak focu,[1]and has at most one limit cycle surrounding a 2nd-order weak fOcus['], study-ing the number of limit cycles of a p1anar quadratic system with a 3rd-order(or 2nd-order) weak focus we only need to study the number of limit cyclessurrounding the strong focus for the system. Without loss of generality thequadratic system with a 3rd--order (or 2nd--order) weak foclls and a strong focuscan be written in the fo.…     

Uniqueness of Limit Cycle for the Quadratic Systems with Weak Saddle and Focus

It is proved that the quadratic system with a weak saddle has at most one limit cycle, and that if this system has a separatrix cycle passing through the weak saddle, then the stability of the separatrix cycle is contrary to that of the singular point surrounded by it.     

Uniqueness of Limit Cycle for the Quadratic Systems with Weak Saddle and Focus

It is proved that the quadratic system with a weak saddle has at most one limit cycle,andthat if this system has a separatrix cycle passing through the weak saddle,then the stability of theseparatrix cycle is contrary to that of the singular point surrounded by it.     

THE MAXIMAL NUMBER OF LIMIT CYCLES FOR QUADRATIC DIFFERENTIAL SYSTEM  = -y + lx~2 + xy,  = x(l + ax + by)

In this paper, we investigate the maximal number of limit cycles surrounding a first order weak focus for the quadratic differential system. And proved such a system has at most two limit cycles under some certain conditions.     

An Important Property of the Weak Focus of a Quadratic Differential System

It was proved in [1] that the order of a weak focus of a quadratic differential system is at most3,i.e.,if v_1=v_3=v_5=v_7=0 in Bautin's symbol,then the critical point is a center.By using theDulac function method we prove in this paper that,if a quadratic differential system has two weakfoci,then each focus must be of order 1;and also a known result of L.A.Cherkas:under the aloveconditon no limit cycle can exist.     

THE UNIQUENESS OF LIMIT CYCLE AND THE STRUCTURE OF CRITICAL POINT AT INFINITY FOR A CLASS OF CUBIC SYSTEM

A class of cubic system, which is an accompany system of a quadratic differential one, is studied. It is proved that the system has at most one limit cycle, and the critical point at infinity is a higher order one. The structure and algebraic character of the critical point at infinity are obtained.     

A CLASS OF QUADRATIC DIFFERENTIAL SYSTEM WITH A THIRD ORDER WEAK FOCUS

This paper discusses the uniqueness of the limit cycle of quadratic differential system with a third order weak focus.     

NON-EXISTENCE OF LIMIT CYCLE AROUND A WEAK FOCUS OF ORDER THREE FOR ANY QUADRATIC SYSTEM

In 1980 Professor Ye Yangian proposed a conjecture that around a weak focus oforder 3 of any real quadratic differential system there can exist no limit cycle.It is thepurpose of this paper to give a proof of the conjecture by using the method of continuousvariation of a coefficient.     

NUMBER OF LIMIT CYCLES OF THE BOUNDED QUADRATIC SYSTEM WITH TWO FINITE SINGULAR POINTS

In this paper, the author proves the bounded quadratic system with two singular points at finite which corresponds to figures 12(a), 12(b), and 13(b) in[1] has at most one limit cycle, and shows under what conditions the limit cycle exists.     

一类具细焦点的三次系统极限环的唯一性

继续相关文献的工作,给出与二次系统Ⅰ相伴的一类三次系统在奇点N(0,1/n)的焦点量公式,证明了系统在细焦点N外围至多有一个极限环,同时证明了当N或O为细焦点时,系统在另一个焦点外围无极限环,结合相关文献的结论,说明了具有细焦点的该系统在全平面至多有一个极限环.     

Hopf Cyclicity of a Family of Generic Reversible Quadratic Systems with One Center

This paper is concerned with small quadratic perturbations to one parameter family of generic reversible quadratic vector fields with a simple center. The first objective is to show that this system exhibits two small amplitude limit cycles emerging from a Hopf bifurcation. The second one we prove that the system has no limit cycle around the weak focus of order two. The results may be viewed as a contribution to proving the conjecture on cyclicity proposed by Iliev (1998).     

二次系统二阶细焦点外围极限环的唯一性

本文证明了平面二次系统二阶细焦点外围至多存在一个极限环这一猜想,并证明了若第二、第三焦点量的乘积大于零,则在二阶细焦点外围不存在极限环．     

一类三次系统的极限环个数与奇点分支

给出二次系统I的一类相伴系统在奇点O(0,0)的焦点量公式,证明了O至多为2阶细焦点,δlmn=0时系统在O外围至多有一个极限环,从而说明了系统在细焦点外围至多有一个极限环。最后给出了各个奇点的分支情况及几何特征。     

一类具有二阶细焦点的二次系统

本文证明了一类具有二阶细焦点的二次系统（在其二阶细焦点外围）至多存在一个极限环．     

二次系统(Ⅲ)n=0一阶细焦点外围极限环的惟一性

本文证明二次系统（Ⅲ）n=0方程当其细焦点的一阶细焦点量（w1)和三阶细焦点量（w3)的符号异号时,该细焦点外围至多有一个极限环;当ω1与ω3符号相同时,该细焦点外围可以出现二个极限环,并举出例子。ω