Abstract
The use of tsumexp(iS[x]) is the generic form for a sum over histories in configuration space is discussed critically and placed in its proper context. The standard derivation of the sum over paths by discretizing the paths is reviewed, and it is shown that the form tsumexp(iS[x]) is justified only for Schrödinger-type systems which are at most second order in the momenta. Extending this derivation to the relativistic free particle, the causal Green’s function is expressed as a sum over timelike paths, and the Feynman Green’s function is expressed both as a sum over paths which only go one way in time and as a sum over paths which move forward and backward in time. The weighting of the paths is shown not to be exp(iS[x]) is any of these cases. The role of the inner product and the operator ordering of the wave equation in defining the sum over histories is discussed.
- Received 13 August 1993
DOI:https://doi.org/10.1103/PhysRevD.49.4049
©1994 American Physical Society