From a QM (not QFT) context, one particle, we start with a hamiltonian H(q,p) and develop something like
\langle q'',T|q',0\rangle \approx \int e^{-i\sum_{l=0}^{N}[H(q_l,p_l)-p_l\dot{q}_l]\delta t}\prod_{j=1}^N{dq_j}\prod_{j=0}^N{\frac{dp_k}{2\pi}}
where \delta t = T/(N+1) and \dot{q}_j...