Abstract
By introducing the family of Feynman maps Fs, we show that our earlier definition of the Feynman path integral F=F1 can be obtained as the analytic continuation of the Wiener integral E =Fi. This leads to some new results for the Wiener and Feynman integrals. We establish a translation and Cameron–Martin formula for the Feynman maps Fs, having applications to nonrelativistic quantum mechanics. We also estalish a (weak) dominated convergence theorem for F1=F.

This publication has 12 references indexed in Scilit: