  A general procedure for constructing coherent states, which are eigenstates
of annihilation operators, related to quantum mechanical potential problems, is
presented. These coherent states, by construction are not potential specific
and rely on the properties of the orthogonal polynomials, for their derivation.
The information about a given quantum mechanical potential enters into these
states, through the orthogonal polynomials associated with it and also through
its ground state wave function. The time evolution of some of these states
exhibit fractional revivals, having relevance to the factorization problem.
