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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