<p>In this paper we investigate the planar circular restricted (<InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(3 + 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>3</mn> <mo>+</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>)-body problem. A massless particle moves under the Newtonian gravitational influence of three primaries. These primaries revolve in circular orbits around their common center of mass within the same plane, forming a collinear configuration. We establish the existence and nonlinear stability of equilibrium points under the condition that two of the primaries have equal masses, denoted by <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>μ</mi> </math></EquationSource> </InlineEquation>. Through analytical and numerical methods, we identify a critical mass parameter <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mu _1 \approx 0.0743\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>μ</mi> <mn>1</mn> </msub> <mo>≈</mo> <mn>0.0743</mn> </mrow> </math></EquationSource> </InlineEquation> where a Hamiltonian–Hopf bifurcation occurs at non-collinear equilibrium points. Furthermore, we prove the existence of Hill-type periodic orbits and KAM tori surrounding these periodic orbits in this circular restricted four-body problem.</p>

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Hamiltonian–Hopf Bifurcation and KAM Tori for the Restricted Four-Body Problem

  • Xuemei Li,
  • Qiyao Mai

摘要

In this paper we investigate the planar circular restricted ( \(3 + 1\) 3 + 1 )-body problem. A massless particle moves under the Newtonian gravitational influence of three primaries. These primaries revolve in circular orbits around their common center of mass within the same plane, forming a collinear configuration. We establish the existence and nonlinear stability of equilibrium points under the condition that two of the primaries have equal masses, denoted by \(\mu \) μ . Through analytical and numerical methods, we identify a critical mass parameter \(\mu _1 \approx 0.0743\) μ 1 0.0743 where a Hamiltonian–Hopf bifurcation occurs at non-collinear equilibrium points. Furthermore, we prove the existence of Hill-type periodic orbits and KAM tori surrounding these periodic orbits in this circular restricted four-body problem.