In the setting of Cameron and
Storvick’s recent theory we show that the solution of an integral equation
formally equivalent to the Schroedinger equation is expressible as the analytic
Feynman integral of a function on ν-dimensional Wiener space of the form
F(X) =exp{∫0t𝜃(t − s,X(s) +ξ)ds}ψ(X(t) +ξ). Here X is an Rν-valued
continuous function on [0,t] such that X(0) =0, ξ∈ Rν, and ψ and 𝜃(s,⋅) are
Fourier-Stieltjes transforms.