English

Solution of the parametric center problem for the Abel differential equation

Classical Analysis and ODEs 2014-07-02 v1 Dynamical Systems

Abstract

The Abel differential equation y=p(x)y2+q(x)y3y'=p(x)y^2+q(x)y^3 with p,qR[x]p,q\in \mathbb R[x] is said to have a center on a segment [a,b][a,b] if all its solutions, with the initial value y(a)y(a) small enough, satisfy the condition y(b)=y(a)y(b)=y(a). The problem of description of conditions implying that the Abel equation has a center may be interpreted as a simplified version of the classical Center-Focus problem of Poincar\'e. The Abel equation is said to have a "parametric center" if for each εR\varepsilon \in \mathbb R the equation y=p(x)y2+εq(x)y3y'=p(x)y^2+\varepsilon q(x)y^3 has a center. In this paper we show that the Abel equation has a parametric center if and only if the antiderivatives P=p(x)dx,P=\int p(x) dx, Q=q(x)dxQ=\int q(x) dx satisfy the equalities P=P~W, P=\widetilde P \circ W,\ Q=Q~WQ=\widetilde Q\circ W for some polynomials P~,\widetilde P, Q~,\widetilde Q, and WW such that W(a)=W(b)W(a)=W(b). We also show that the last condition is necessary and sufficient for the "generalized moments" abPidQ\int_a^b P^id Q and abQidP\int_a^b Q^id P to vanish for all i0.i\geq 0.

Cite

@article{arxiv.1407.0150,
  title  = {Solution of the parametric center problem for the Abel differential equation},
  author = {Fedor Pakovich},
  journal= {arXiv preprint arXiv:1407.0150},
  year   = {2014}
}
R2 v1 2026-06-22T04:52:12.086Z