Special rectangular (double-well and hole) potentials
Abstract
We revisit a rectangular barrier as well as a rectangular well (pit) between two rigid walls. The former is the well known double-well potential and the latter is a hole potential. Let |V0| be the height (depth) of the barrier (well) then for a fixed geometry of the potential, we show that in the double-well, E=V0(>0), and in the hole potential (V0 <0), E=0, can be energy eigenvalues provided V0 admits some special discrete values. These states have been missed out earlier which emerge only when one seeks the special zero-energy solution of one-dimensional Schr\"odinger equation as (x)=Bx+C.
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