2020
DOI: 10.1007/s11071-020-05795-0
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Relaxation oscillations and the mechanism in a periodically excited vector field with pitchfork–Hopf bifurcation

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Cited by 21 publications
(3 citation statements)
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“…two scales in frequency domain, bursting oscillations can also be observed, while the bursting mechanism can't be obtained directly by the traditional slow-fast analysis method. In recent years, Bi et al [7,[26][27][28] presented a modified slow-fast method with the conceptions of generalized autonomous system and transformed phase portrait, which have been demonstrated to be an effective tool to analyze the generation mechanism of bursting oscillations in dynamical systems with a single slow excitation. The one periodic excitation dynamical systems can be expressed in the form ẋ = f[x, µ µ µ, Acos(ωt)],…”
Section: Introductionmentioning
confidence: 99%
“…two scales in frequency domain, bursting oscillations can also be observed, while the bursting mechanism can't be obtained directly by the traditional slow-fast analysis method. In recent years, Bi et al [7,[26][27][28] presented a modified slow-fast method with the conceptions of generalized autonomous system and transformed phase portrait, which have been demonstrated to be an effective tool to analyze the generation mechanism of bursting oscillations in dynamical systems with a single slow excitation. The one periodic excitation dynamical systems can be expressed in the form ẋ = f[x, µ µ µ, Acos(ωt)],…”
Section: Introductionmentioning
confidence: 99%
“…two scales in frequency domain, bursting oscillations can also be observed, while the bursting mechanism can't be obtained directly by the traditional slow-fast analysis method. In recent years, Bi et al [7,[26][27][28] presented a modified slow-fast method with the conceptions of generalized autonomous system and transformed phase portrait, which have been demonstrated to be an effective tool to analyze the generation mechanism of bursting oscillations in dynamical systems with a single slow excitation. The one periodic excitation dynamical systems can be expressed in the formẋ = f[x, µ µ µ, Acos(ωt)],…”
Section: Introductionmentioning
confidence: 99%
“…Ambrosio et al addressed the canard phenomenon in a slow-fast modified Leslie-Gower model [20]. Xia et al discussed relaxation oscillations and the mechanism in a periodically excited vector field with pitchfork-Hopf bifurcation [21]. Atabaigi and Barati studied relaxation oscillations and canard explosion in a predatorprey system of Holling and Leslie types [22].…”
Section: Introductionmentioning
confidence: 99%