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Up to the first two order Melnikov analysis for the exact cyclicity of planar piecewise linear vector fields with nonlinear switching curve.

Authors :
Zhao, Liqin
Si, Zheng
Jia, Ranran
Source :
Journal of Differential Equations. Jan2025:Part 3, Vol. 416, p2255-2292. 38p.
Publication Year :
2025

Abstract

In this paper, we focus on providing the exact bounds for the maximum number of limit cycles Z (3 , n) that planar piecewise linear differential systems with two zones separated by the curve y = x 3 under perturbation of arbitrary polynomials of x , y with degree n can have, where n ∈ N. By the first two order Melnikov functions, we achieve that Z (3 , 2) = 12 , Z (3 , n) = 2 n + 1 for 3 ≤ n ≤ 88 and Z (3 , n) ≥ 2 n + 1 for any n. The results are novel and improve the previous results in the literature. • We achieved a result about the coexistence of small amplitude and big amplitude limit cycles in Lemma 3.6 (see P 18), which yields system (1.1) ϵ can have 2 n small amplitude limit cycles simultaneously a large one for n odd. • We got a good way to avoid finding the zero points of the Wronskians in applying the useful algebraic method developed in [20]. Specifically, although [26] proved that (F 3) (which is the generating functions of M 1 (u)) is an ECT-system with accuracy 1 for n = 1 , 3 , 5 , it is impossible to find the zero points of the Wronskians for general n. We constructed an auxiliary ordered set of functions (F 2) ⊃ (F 3) (see (3.38) on P 19 and Lemma 3.7) so that we avoided these troubles. In fact, we have checked each Wronskians of (F 2) is non-vanishing since they have the form of M × P (v) v m / 2 (v > 0) , where M , m ≠ 0 are some constants and P (v) are some polynomials of v 2 with positive coefficients. Thus, we achieved Z (3 , n) ≤ 2 n + 1 for n ≤ 88 odd. • We obtained the expression of M 2 (u) without any restriction on perturbation parameters in Lemma 4.1, see P 25. So we can obtain the exact value of Z (3 , 2) = 12 , which improves the result Z (3 , 2) ≥ 5 in [9]. • We performed a transformation in Lemma 3.7 on P 19 so that the calculations of Wronskians are reduced greatly, and we chose clearly the perturbation parameters in Lemma 3.8(ii) (see P 20) such that the corresponding system (1.1) ϵ has at least 2 n + 1 limit cycles. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00220396
Volume :
416
Database :
Academic Search Index
Journal :
Journal of Differential Equations
Publication Type :
Academic Journal
Accession number :
181190749
Full Text :
https://doi.org/10.1016/j.jde.2024.11.007