Feynman's path integral is:
\[
\int {Dx\,e^{{\textstyle{i \over \hbar }}\int {L(x,\dot x,t)dt} } }
\]
where the Action is:
\[
\int {L(x,\dot x,t)dt}
\]
and the Lagrangian is: \[
{L(x,\dot x,t)}
\]
Now we are told that as we functionally integrate the path integral in the...