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Determine the scaling coefficient α governing crisis-induced escape probabilities

Determine the coefficient α in the asymptotic scaling law Q∞(δ) ≈ exp[−α (ln δ)² + β ln δ] for the escape probability near crisis transitions in non-autonomous (time-dependent) dynamical systems, beyond the simple stochastic one-dimensional model where α is linked to the instability of the fixed point whose stable manifold forms the basin boundary; clarify how the attractor’s fractal dimension and temporal correlations of the modulation affect α.

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Background

The paper establishes that crises occur in non-autonomous systems and that the escape probability near the transition follows a nonstandard scaling of the form exp[−α (ln δ)² + β ln δ], where δ is the distance from criticality and α is model-dependent. In the simple linear stochastic grey-zone model, α is related to the instability of a fluctuating saddle that defines the basin boundary.

However, for more complex systems (e.g., stochastically modulated logistic and Hénon maps and the Kuramoto model with inertia), the precise determination of α is left open, with indications that properties such as attractor fractal dimension and temporal correlations likely influence α. The authors explicitly state this as future work.

References

How to determine α? In the simple stochastic one-dimensional model, it is linked to the instability of the fixed point whose stable manifold determines the boundary of the basin of attraction. More in general, we can imagine that the fractal dimension of the attractor to enter as well and the correlations probably play a crucial role. This is left to future work.

Crisis in time-dependent dynamical systems (2503.13152 - Olmi et al., 17 Mar 2025) in Conclusions paragraph