Fig. 3
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Response to a first-order resonance. Left panel: maximum eccentricity, emax, reached by a particle initially on a circular orbit with modified semimajor axis ∆ā/a0, with m < 0 and ϵ′ < 0. The right (resp. left) branch of the function is given by Eq. (29) (resp. 30). The value of emax suffers a discontinuity at Δā/a0 = (3/2)(m − 1)|2ϵ′|2/3, where emax jumps from |2ϵ′|1/3 to |16ϵ′|1/3, the maximum possible eccentricity, epeak. Right panel: phase portrait corresponding to the discontinuity, with the homoclinic trajectory going through the origin. The red and blue points correspond to their counterparts shown in the left panel.
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