
The goal of this paper is to characterize those quadratic differential equations in the plane having a polynomial first integral, and to provide an explicit expression of these systems as well as of their polynomial first integrals. It is well known that if the system writes as \[ \dot x=P(x,y), \quad \dot y=Q(x,y) \] it is not restrictive to assume that \(P(x,y)\in\{1+xy, xy, y+x^2, y, 1+x^2, -1+x^2, x^2, x, 1, 0\}\) and \(Q(x,y)=a+bx+cy+dx^2+exy+fy^2.\) The authors consider only the cases where the system has finitely many critical points and solve completely the problem. For instance, their result when \(P(x,y)=1+x^2\) says that in this case the system has a polynomial first integral \(H(x,y)\) if and only if, either \(f=c=b=d=0,\) \(e=-2k\) with \(k\) a positive integer and \(a=1,\) and then \[ H(x,y)=y(1+x^2)^k-\sum_{j=0}^{k-1}{{k-1}\choose{j}}{{x^{2j+1}}\over{2j+1}}, \] or \(f=a=c=b=d=0\) and \(e=-p/q\) being a negative rational number, and then \(H(x,y)=(1+x^2)^py^{2q}.\) The more complicated cases in their study are the more generic ones, \textit{i.e.} \(P(x,y)=1+xy\) and \(P(x,y)=xy.\)
Dynamics induced by flows and semiflows, Explicit solutions, first integrals of ordinary differential equations, Polynomial first integral, Topological structure of integral curves, singular points, limit cycles of ordinary differential equations, quadratic differential equation, Symmetries, invariants of ordinary differential equations, polynomial first integral, Analysis, Quadratic vector fields
Dynamics induced by flows and semiflows, Explicit solutions, first integrals of ordinary differential equations, Polynomial first integral, Topological structure of integral curves, singular points, limit cycles of ordinary differential equations, quadratic differential equation, Symmetries, invariants of ordinary differential equations, polynomial first integral, Analysis, Quadratic vector fields
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