Metastable decay exhibits a familiar exponential regime bracketed by early-time deviations and late-time power-law tails. We adopt the real-time, flux-based definition of the decay rate in the spirit of Andreassen et al.\ direct method and present a complete analysis of one-dimensional quantum-mechanical resonance models. We show that the kernel admits a universal pole–plus–branch decomposition and use it to define two computable time scales: a dawn time, when a single resonant contribution starts dominating and exponential decay sets in, and a twilight time, when the branch-cut tail overtakes exponential decay. The latter can be expressed in closed form via the Lambert function, making its parametric dependence manifest without fitting. For square, modified square, and Pöschl–Teller barriers we obtain simple thick-barrier formulas, clarify the relation between the decay rate , oscillation period , and transmission probability , and indicate how our spectral picture can be naturally extended to quantum field theoretic vacuum decay.

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