After the free particle, the most elementary example of a one-dimensional time-independent Schrödinger equation is conceptually that of a particle in a delta function potential:
(in units with
). For an attractive potential, with
, there is exactly one bound state, with
and
. Note that
and
. Since the delta function has dimensions of
, this solution is considered the one-dimensional analog of a hydrogen-like atom. The bound state, in fact, resembles a cross section of a 1
orbital
.
For
, free particles are scattered by a delta function potential. The positive-energy solutions can be written
, with
. The amplitudes of the transmitted and reflected waves are accordingly given by
and
, respectively. Note that these are the same for attractive and repulsive delta funtion potentials, independent of the sign of
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