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Dynamical entropy of the separatrix map. / Шевченко, Иван Иванович.

In: Physical Review E, Vol. 111, No. 3, 034211, 17.03.2025.

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@article{dbaf95679b45418cadd9103db19bd987,
title = "Dynamical entropy of the separatrix map",
abstract = "We calculate the maximum Lyapunov exponent of the motion in the separatrix map's chaotic layer, along with calculation of its width, as functions of the adiabaticity parameter 휆. The separatrix map is set in natural variables, and the case of the layer's least perturbed border is considered, i.e., the winding number of the layer's border (the last invariant curve) is the golden mean. Although these two dependences (for the Lyapunov exponent and the layer width) are strongly nonmonotonous and evade any simple analytical description, the calculated dynamical entropy ℎ turns out to be a close-to-linear function of 휆. In other words, if normalized by 휆, the entropy is a quasiconstant. We discuss whether the function ℎ⁡(휆) can be in fact exactly linear, ℎ∝휆. The function ℎ⁡(휆) forms a basis for calculating the dynamical entropy for any perturbed nonlinear resonance in the first fundamental model, as soon as the corresponding Melnikov-Arnold integral is estimated.",
author = "Шевченко, {Иван Иванович}",
year = "2025",
month = mar,
day = "17",
doi = "10.1103/physreve.111.034211",
language = "English",
volume = "111",
journal = "Physical Review E - Statistical, Nonlinear, and Soft Matter Physics",
issn = "1539-3755",
publisher = "American Physical Society",
number = "3",

}

RIS

TY - JOUR

T1 - Dynamical entropy of the separatrix map

AU - Шевченко, Иван Иванович

PY - 2025/3/17

Y1 - 2025/3/17

N2 - We calculate the maximum Lyapunov exponent of the motion in the separatrix map's chaotic layer, along with calculation of its width, as functions of the adiabaticity parameter 휆. The separatrix map is set in natural variables, and the case of the layer's least perturbed border is considered, i.e., the winding number of the layer's border (the last invariant curve) is the golden mean. Although these two dependences (for the Lyapunov exponent and the layer width) are strongly nonmonotonous and evade any simple analytical description, the calculated dynamical entropy ℎ turns out to be a close-to-linear function of 휆. In other words, if normalized by 휆, the entropy is a quasiconstant. We discuss whether the function ℎ⁡(휆) can be in fact exactly linear, ℎ∝휆. The function ℎ⁡(휆) forms a basis for calculating the dynamical entropy for any perturbed nonlinear resonance in the first fundamental model, as soon as the corresponding Melnikov-Arnold integral is estimated.

AB - We calculate the maximum Lyapunov exponent of the motion in the separatrix map's chaotic layer, along with calculation of its width, as functions of the adiabaticity parameter 휆. The separatrix map is set in natural variables, and the case of the layer's least perturbed border is considered, i.e., the winding number of the layer's border (the last invariant curve) is the golden mean. Although these two dependences (for the Lyapunov exponent and the layer width) are strongly nonmonotonous and evade any simple analytical description, the calculated dynamical entropy ℎ turns out to be a close-to-linear function of 휆. In other words, if normalized by 휆, the entropy is a quasiconstant. We discuss whether the function ℎ⁡(휆) can be in fact exactly linear, ℎ∝휆. The function ℎ⁡(휆) forms a basis for calculating the dynamical entropy for any perturbed nonlinear resonance in the first fundamental model, as soon as the corresponding Melnikov-Arnold integral is estimated.

UR - https://www.mendeley.com/catalogue/4c2f1088-f47a-3dee-abf9-227cacb9659b/

U2 - 10.1103/physreve.111.034211

DO - 10.1103/physreve.111.034211

M3 - Article

VL - 111

JO - Physical Review E - Statistical, Nonlinear, and Soft Matter Physics

JF - Physical Review E - Statistical, Nonlinear, and Soft Matter Physics

SN - 1539-3755

IS - 3

M1 - 034211

ER -

ID: 133165148