TY - JOUR
T1 - Limit Cycles in a Class of Planar Discontinuous Piecewise Quadratic Differential Systems with a Non-regular Line of Discontinuity (II)
AU - He, Dongping
AU - Llibre, Jaume
N1 - Publisher Copyright:
© The Author(s), under exclusive licence to Springer Nature Switzerland AG 2024.
PY - 2024/8/20
Y1 - 2024/8/20
N2 - In our previous work, we have studied the limit cycles for a class of discontinuous piecewise quadratic polynomial differential systems with a non-regular line of discontinuity, which is formed by two rays starting from the origin and forming an angle α=π/2. The unperturbed system is the quadratic uniform isochronous center x˙=-y+xy, y˙=x+y2 with a family of periodic orbits surrounding the origin. In this paper, we continue to investigate this kind of piecewise differential systems, but now the angle between the two rays is α∈(0,π/2)∪[3π/2,2π). Using the Chebyshev theory, we prove that the maximum number of hyperbolic limit cycles that can bifurcate from these periodic orbits using the averaging theory of first order is exactly 8 for α∈(0,π/2)∪[3π/2,2π). Together with our previous work, which concerns on the case of α=π/2, we can conclude that using the averaging theory of first order the maximum number of hyperbolic limit cycles is exactly 8, when this quadratic center is perturbed inside the above-mentioned classes separated by a non-regular line of discontinuity with α∈(0,π/2]∪[3π/2,2π).
AB - In our previous work, we have studied the limit cycles for a class of discontinuous piecewise quadratic polynomial differential systems with a non-regular line of discontinuity, which is formed by two rays starting from the origin and forming an angle α=π/2. The unperturbed system is the quadratic uniform isochronous center x˙=-y+xy, y˙=x+y2 with a family of periodic orbits surrounding the origin. In this paper, we continue to investigate this kind of piecewise differential systems, but now the angle between the two rays is α∈(0,π/2)∪[3π/2,2π). Using the Chebyshev theory, we prove that the maximum number of hyperbolic limit cycles that can bifurcate from these periodic orbits using the averaging theory of first order is exactly 8 for α∈(0,π/2)∪[3π/2,2π). Together with our previous work, which concerns on the case of α=π/2, we can conclude that using the averaging theory of first order the maximum number of hyperbolic limit cycles is exactly 8, when this quadratic center is perturbed inside the above-mentioned classes separated by a non-regular line of discontinuity with α∈(0,π/2]∪[3π/2,2π).
KW - 34C05
KW - 34C07
KW - 34C25
KW - 34C29
KW - Chebyshev theory
KW - Limit cycle
KW - averaging theory
KW - discontinuous piecewise polynomial system
KW - non-regular line of discontinuity
KW - quadratic uniform isochronous center
UR - https://www.scopus.com/pages/publications/85201541974
UR - https://www.mendeley.com/catalogue/305913ff-7dc7-3e5b-aee2-a769459bc721/
U2 - 10.1007/s00009-024-02714-0
DO - 10.1007/s00009-024-02714-0
M3 - Article
SN - 1660-5446
VL - 21
JO - Mediterranean Journal of Mathematics
JF - Mediterranean Journal of Mathematics
IS - 6
M1 - 174
ER -