Integration by parts formulas involving generalized Fourier-Feynman transforms on function space

Author:

Chang Seung,Choi Jae,Skoug David

Abstract

In an upcoming paper, Chang and Skoug used a generalized Brownian motion process to define a generalized analytic Feynman integral and a generalized analytic Fourier-Feynman transform. In this paper we establish several integration by parts formulas involving generalized Feynman integrals, generalized Fourier-Feynman transforms, and the first variation of functionals of the form F ( x ) = f ( α 1 , x , , α n , x ) F(x)=f(\langle \alpha _{1} , x\rangle , \dots , \langle \alpha _{n} , x\rangle ) where α , x \langle {\alpha ,x}\rangle denotes the Paley-Wiener-Zygmund stochastic integral 0 T α ( t ) d x ( t ) \int _{0}^{T} \alpha (t) d x(t) .

Publisher

American Mathematical Society (AMS)

Subject

Applied Mathematics,General Mathematics

Reference13 articles.

1. An 𝐿₂ analytic Fourier-Feynman transform;Cameron, R. H.;Michigan Math. J.,1976

2. Feynman integral of variations of functionals;Cameron, R. H.,1991

3. Fourier-Feynman transform, convolution and first variation of functionals on abstract Wiener space;Chang, K. S.;Integral Transform. Spec. Funct.,2000

4. [4] S. J. Chang and D. L. Skoug, The effect of drift on the Fourier-Feynman transform, the convolution product and the first variation, Panamerican Math. J. 10 (2000), 25-38.

5. [5] \bysame, Generalized Fourier-Feynman transforms and a first variation on function space, to appear in Integral Transforms and Special Functions.

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