The quantum mechanical problem of a particle moving in one dimension (
1D) under the influence of a singular potential is reexamined. An attr
active delta function potential of infinite strength and the 1D Coulom
b potential is considered in particular. In both cases the singularity
acts as an impenetrable barrier, thus dividing space into two indepen
dent regions. Analysis of the scattering states gives results in agree
ment with this conclusion. The implications that the bound states of t
he 1D Coulomb potential cannot be classified according to parity, even
though the potential is symmetric, is also discussed herein.