Conventional path integral expressions for propagators are representat
ion dependent. Rather than having to adapt each propagator to the repr
esentation in question, it is shown that for compact Lie groups it is
possible to introduce a propagator that is representation independent.
For a given set of kinematical variables this propagator is a single
function independent of any particular choice of fiducial vector, whic
h monetheless, correctly propagates each element of the coherent state
representation associated with these kinematical variables. Although
the configuration space is in general curved, nevertheless the lattice
phase-space path integral for the representation independent propagat
or has the form appropriate to flat space. To illustrate the general t
heory a representation independent propagator is explicitly constructe
d for the Lie group SU(2).