Solution of the parametric center problem for the Abel differential equation

preprint2014arXivOpen access

Abstract

The Abel differential equation y′=p(x)y2+q(x)y3y'=p(x)y^2+q(x)y^3 with p,q∈R[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 Poincaré. The Abel equation is said to have a "parametric center" if for each ε∈R\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 i≥0.i\geq 0.

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