2017
DOI: 10.1007/s10958-017-3221-y
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Typicality of Chaotic Fractal Behavior of Integral Vortices in Hamiltonian Systems with Discontinuous Right Hand Side

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Cited by 11 publications
(9 citation statements)
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“…Blowing up the singularity. To prove Theorem 3.2 we use the procedure of resolution of singularity for the Hamiltonian system (7) [54,51]. Consider the blowing up the singularity at the origin by the map B : z → (µ,z):…”
Section: 3mentioning
confidence: 99%
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“…Blowing up the singularity. To prove Theorem 3.2 we use the procedure of resolution of singularity for the Hamiltonian system (7) [54,51]. Consider the blowing up the singularity at the origin by the map B : z → (µ,z):…”
Section: 3mentioning
confidence: 99%
“…Let Q denote the cylinder {µ ∈ R} × Π, and Q 0 = Q ∩ {µ = 0}. It was proved [54] that B is a diffeomorphism from R 8 \ {0} onto Q ∩ {µ > 0}. In the coordinates (µ,z) the system (7) has the form:…”
Section: 3mentioning
confidence: 99%
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“…Often optimal trajectories consist of nonsingular and singular arcs and the concatenation structures of these arcs can be very irregular, for example, the chattering or the Fuller phenomenon (an infinite number of control discontinuities in a finite time interval) [17,20,22,26,33,34], iterated Fuller singularities [35], a chaotic behaviour of bounded pieces of optimal trajectories [36]. Such structure of optimal controls, rather complicated from a mathematical point of view, is very typical for controlling systems that possess singular regimes.…”
Section: Introductionmentioning
confidence: 99%