1999
DOI: 10.1088/0951-7715/12/2/010
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Change of the adiabatic invariant at a separatrix in a volume-preserving 3D system

Abstract: A 3D volume-preserving system is considered. The system differs by a small perturbation from an integrable one. In the phase space of the unperturbed system there are regions filled with closed phase trajectories, where the system has two independent first integrals. These regions are separated by a 2D separatrix passing through nondegenerate singular points. Far from the separatrix, the perturbed system has an adiabatic invariant. When a perturbed phase trajectory crosses the two-dimensional separatrix of the… Show more

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Cited by 48 publications
(96 citation statements)
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“…The change of the adiabatic invariant due to separatrix crossing is estimated applying Neishtadt's theory [3][4][5], since the IAI (9) tends to the IAI of the interpolating Hamiltonian. Moreover, the evolution of the frozen energy H(ρ, ψ, λ) = E and of the scaled period ǫ T (J, λ) can be described by the dynamics of the interpolating Hamiltonian up to an error O(ǫ 2 ).…”
Section: B Trapping Into Resonance and Change Of Adiabatic Invariantmentioning
confidence: 99%
“…The change of the adiabatic invariant due to separatrix crossing is estimated applying Neishtadt's theory [3][4][5], since the IAI (9) tends to the IAI of the interpolating Hamiltonian. Moreover, the evolution of the frozen energy H(ρ, ψ, λ) = E and of the scaled period ǫ T (J, λ) can be described by the dynamics of the interpolating Hamiltonian up to an error O(ǫ 2 ).…”
Section: B Trapping Into Resonance and Change Of Adiabatic Invariantmentioning
confidence: 99%
“…The asymptotic formulas for the jump of adiabatic invariant on a separatrix were obtained by Timofeev (Timofeev, 1978) for particular case of a pendulum in a slowly varying gravity field, by Neishtadt (Neishtadt, 1986) and Cary and co-workers (Cary et al, 1986) for systems with one degree of freedom plus slowly varying parameter and by Neishtadt (Neishtadt, 1987) for systems with two degrees of freedom, one corresponding to the fast motion and the other corresponding to the slow motion. This theory was first applied to magnetospheric problems in (Büchner and Zelenyi, 1989).…”
Section: Separatrix Crossingsmentioning
confidence: 99%
“…The variables of the classical Hamiltonian are defined as (17) into the time-dependent GP equation, one gets [38] i dψ 1 …”
Section: Nonlinear Two-mode Model For Two Coupled Becmentioning
confidence: 99%
“…A conceptual phenomenon of classical adiabatic theory is destruction of adiabatic invariance at separatrix crossings which is encountered, in particular, in plasma physics and hydrodynamics, classical and celestial mechanics [10,11,12,13,14,15,16,17,18,19,20,21,22]. The phenomenon is very important for BEC physics: we consider here nonlinear two-mode models related to tunnelling between coupled BEC in a double well [23], nonlinear Landau-Zener tunnelling [24,25], Feshbach resonance passage in atom-molecule systems [26,27,28].…”
Section: Introductionmentioning
confidence: 99%
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