Path-integral expressions for one-particle propagators in scalar and f
ermionic field theories are derived, for arbitrary mass. This establis
hes a direct connection between field theory and specific classical po
int-particle models. The role of world-line reparametrization invarian
ce of the classical action and the implementation of the corresponding
BRST symmetry in the quantum theory are discussed. The presence of cl
assical world-line supersymmetry is shown to lead to an unwanted doubl
ing of states for massive spin-1/2 particles. The origin of this pheno
menon is traced to a ''hidden'' topological fermionic excitation. A di
fferent formulation of the pseudo-classical mechanics using a bosonic
representation of ys is shown to remove these extra states at the expe
nse of losing manifest supersymmetry.