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Kirkwood gaps and diffusion along mean motion resonances in the restricted planar three-body problem

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Academic year: 2021

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Figure 2: Transition from the instant ellipse of eccentricty e = 0.48 to the instant ellipse of eccentricty e = 0.67
Figure 3: The diffusion path that we study in the (a, e) plane. The horizontal lines represent the resonances along which we drift
Figure 4: The periodic orbit obtained for every energy level intersects the Poincar´e section {g = 0} seven times, as shown schematically in this picture
Figure 5: Resonant periodic orbit λ −1.6 of the circular problem in rotating Cartesian coordinates.
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