Abstract

Hitherto, a finitely thick barrier next to a well or a rigid wall has been considered the potential of simplest shape giving rise to resonances (metastable states) in one dimension: x∈(−∞,∞)x \in(-\infty, \infty). In such a potential, there are three real turning points at an energy below the barrier. Resonances are Gamow's (time-wise) decaying states with discrete complex energies (En=En−iΓn/2)({\cal E}_n = E_n -iΓ_n/2). These are also spatially catastrophic states that manifest as peaks/wiggles in Wigner's reflection time-delay at E=εn≈EnE = ε_n \approx E_n. Here we explore potentials with simpler shapes giving rise to resonances - two-piece rising potentials having just one-turning point. We demonstrate our point by using rising exponential profile in various ways.

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