To be used in future
 Section 5.9: Brownian Motion Up Chapter 5: Path Integrals Section 5.11: Partition sum 

5.10 Time-ordered Perturbation Theory

Let We assume we know the propagtor for . We get We expand in powers of , and get Taylor expanding, we find that We now use the trick that we can order the time integration variables in different ways to put them in increasing order of time and find that We now split into the same time intervals, and find that This is the basic equation of time-ordered perturbation theory.
There is a very neat alternative way to write this expression
 Section 5.9: Brownian Motion Up Chapter 5: Path Integrals Section 5.11: Partition sum