2019
DOI: 10.1016/j.geomphys.2019.103493
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Bifurcations and monodromy of the axially symmetric 1:1:2 resonance

Abstract: We consider integrable Hamiltonian systems in three degrees of freedom near an elliptic equilibrium in 1:1:−2 resonance. The integrability originates from averaging along the periodic motion of the quadratic part and an imposed rotational symmetry about the vertical axis. Introducing a detuning parameter we find a rich bifurcation diagram, containing three parabolas of Hamiltonian Hopf bifurcations that join at the origin. We describe the monodromy of the resulting ramified 3-torus bundle as variation of the d… Show more

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Cited by 5 publications
(3 citation statements)
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“…We stress again that we always consider δ = 0, because adding the additional quadratic term in L 3 to the Hamiltonian deforms the bifurcation diagram, but does not essentially change it. Bifurcations similar to those found here have recently been described in [34,17], in particular also the related quantum monodromy in [34]. Let us start with the ordinary Lagrange top, c 2 = 0 [8].…”
Section: Bifurcation Diagramsupporting
confidence: 79%
“…We stress again that we always consider δ = 0, because adding the additional quadratic term in L 3 to the Hamiltonian deforms the bifurcation diagram, but does not essentially change it. Bifurcations similar to those found here have recently been described in [34,17], in particular also the related quantum monodromy in [34]. Let us start with the ordinary Lagrange top, c 2 = 0 [8].…”
Section: Bifurcation Diagramsupporting
confidence: 79%
“…The approach we take to study the 2:4 resonance has become rather standard, compare with [25,12,20,24,14] and references therein. Normalizing about the periodic flow of the resonant oscillator introduces an extra continuous symmetry, cf.…”
Section: What Is Newmentioning
confidence: 99%
“…Remark 4.3 The simple geometry of the parabola allows to immediately conclude stability or instability of the equilibria and how these come into existence through centre-saddle and Hamiltonian flip bifurcations. The corresponding formulas may as well be searched for as double roots of the difference of the polynomials describing phase space and energy level set [14]. For more involved expressions than the present cubic, which is well approximated by a parabola, an algebraic point of view can support the present geometric approach, relying on the resultant of two polynomials and related tools.…”
Section: Regular Equilibriamentioning
confidence: 99%

On the detuned 2:4 resonance

Hanssmann,
Marchesiello,
Pucacco
2020
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