From the very beginning, coherent state path integrals have always relied o
n a coherent state resolution of unity for their construction. By choosing
an inadmissible fiducial vector, a st of "coherent states" spans the same s
pace but loses its resolution of unity,and for that reason has been called
a set of weak coherent states. Despite having no resolution of unity, it is
nevertheless shown how the propagator in such a basis may admit a phase-sp
ace path integral representation in essentially the same form as if it had
a resolution of unity. Our examples are toy models of similar situations th
at arise in current studies of quantum gravity.