
The authors define the conditional generalized Fourier-Feynman transform and conditional generalized convolution product for functionals on a function space which is rather general than the Wiener space and was introduced by \textit{S. J. Chang} and \textit{D. Skoug} [Integral Transforms Spec. Funct. 14, No. 5, 375--393 (2003; Zbl 1043.28014)]. Then they establish some relationships between the two concepts for functionals which belong to a Banach algebra in the function space. \textit{S. J. Chang} and \textit{D. Skoug} [loc. cit.] used a generalized Brownian motion process to define a generalized analytic Feynman integral and a generalized analytic Fourier-Feynman transform. The Wiener process used by \textit{C. Park} and \textit{D. Skoug} [J. Korean Math. Soc. 38, No. 1, 61--76 (2001; Zbl 1015.28016)] is free of drift and is stationary in time while the stochastic process used in this paper is nonstationary in time and is subject to a drift.
generalized analytic Feynman integral, Path integrals in quantum mechanics, Set functions and measures and integrals in infinite-dimensional spaces (Wiener measure, Gaussian measure, etc.), conditional generalized analytic Fourier-Feynman transform, generalized Brownian motion process, conditional generalized convolution product, Brownian motion, Applications of functional analysis in probability theory and statistics
generalized analytic Feynman integral, Path integrals in quantum mechanics, Set functions and measures and integrals in infinite-dimensional spaces (Wiener measure, Gaussian measure, etc.), conditional generalized analytic Fourier-Feynman transform, generalized Brownian motion process, conditional generalized convolution product, Brownian motion, Applications of functional analysis in probability theory and statistics
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