Center problem for generalized Λ-Ω differential systems

The Λ-Ω differential systems are the real planar polynomial differential equations of degree m of the form ˙ x = -y(1 + Λ) + xΩ, ˙ y = x(1 + Λ) + yΩ, where Λ = Λ(x,y) and Ω = Ω(x,y) are polynomials of degree at most m-1 such that Λ(0,0) = Ω(0,0) = 0. We study the center problem for these Λ-Ω systems...

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Detalhes bibliográficos
Autores: Llibre, Jaume|||0000-0002-9511-5999, Ramírez, Rafael Orlando|||0000-0002-4958-0291, Ramírez, Valentín
Formato: artículo
Fecha de publicación:2018
País:España
Recursos:Universitat Autònoma de Barcelona
Repositorio:Dipòsit Digital de Documents de la UAB
Idioma:inglés
OAI Identifier:oai:ddd.uab.cat:222607
Acesso em linha:https://ddd.uab.cat/record/222607
Access Level:acceso abierto
Palavra-chave:Darboux first integral
Linear type centers
Poincaré-Liapunov Theorem
Reeb integrating factor
Weak center
Descrição
Resumo:The Λ-Ω differential systems are the real planar polynomial differential equations of degree m of the form ˙ x = -y(1 + Λ) + xΩ, ˙ y = x(1 + Λ) + yΩ, where Λ = Λ(x,y) and Ω = Ω(x,y) are polynomials of degree at most m-1 such that Λ(0,0) = Ω(0,0) = 0. We study the center problem for these Λ-Ω systems. A planar vector field with linear type center can be written as an Λ-Ω system if and only if the Poincaré-Liapunov first integral is of the form F = 1 2 (x2 + y2)(1 + O(x,y)). The main objective of this paper is to study the center problem for Λ-Ω systems of degree m with Λ = µ(a2x - a1y), and Ω = a1x + a2y + m-1 ∑ j=2 Ωj, where µ, a1, a2 are constants and Ωj = Ωj(x,y) is a homogenous polynomial of degree j, for j = 2,...,m-1. We prove the following results. Assuming that m = 2,3,4,5 and (µ + (m-2))(a2 1 + a2 2) ̸= 0 and m-2 ∑ j=2 Ωj ̸= 0 then the Λ-Ω system has a weak center at the origin if and only if these systems after a linear change of variables (x,y) -→ (X,Y ) are invariant under the transformations (X,Y,t) -→ (-X,Y,-t). If (µ + (m-2))(a2 1 + a2 2) = 0 and m-2 ∑ j=1 Ωj = 0 then the origin is a weak center. We observe that the main difficulty to prove this result for m.