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Figure 1. The boundary (5) (solid curves) for the potential V = m2ϕ2/2. Points of maximal expansionare located between two dashed curves while bounces are possible in two narrow zones between solid anddashed curves.
Figure 2. Example of trajectories with the initial conditions close to the boundary separating trajectoriesfalling into ϕ = +∞ (trajectory 1) and ϕ = −∞ (trajectories 2–5) singularities for the case ϕ0 <√34√πmP .This boundary is sharp, no fractal structure
Figure 3. TheConsecutive merging of 5 first intervals can be seen in this range of ϕ = 0 cross-section of the bounce intervals for the potential V = m2ϕ2/2 and negative C
Figure 4.The value ϕ0 of the potential (10) corresponding to the first merging of the bounce intervalsdepending on power index q.

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