Ahmed, Z.Pavaskar, S.Prakash, L.2026-02-052015European Journal of Physics, 2015, 36, 4, pp. -1430807https://doi.org/10.1088/0143-0807/36/4/048001https://idr.nitk.ac.in/handle/123456789/26265Hitherto, 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 ?(-?, ?). 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.(?<inf>n</inf> = E<inf>n</inf> - i?<inf>n</inf>/2) These are also spatially catastrophic states that manifest as peaks/wiggles in Wigner's reflection time delay at E = ? ? E<inf>n</inf> 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. © 2015 IOP Publishing Ltd.ResonanceTiming circuitsGamow-siegert decaying stateOne dimensionOne-dimensional scatteringReflection amplitudeRigid wallShape resonanceSimple++Time-delaysTurning-pointsWigne time-delayTime delay