CONDITIONAL INTEGRAL TRANSFORMS AND CONVOLUTIONS OF BOUNDED FUNCTIONS ON AN ANALOGUE OF WIENER SPACE
- 충청수학회
- Journal of the Chungcheong Mathematical Society
- Volume 26, No. 2
-
2013.05323 - 342 (20 pages)
- 2
Let C[0; t] denote the function space of all real-valued continuous paths on [0; t]. De¯ne Xn : C[0; t] ! Rn+1 and Xn+1 : C[0; t] ! Rn+2 by Xn(x) = (x(t0); x(t1); ¢ ¢ ¢ ; x(tn)) and Xn+1(x) =(x(t0); x(t1); ¢ ¢ ¢ ; x(tn); x(tn+1)), where 0 = t0 < t1 < ¢ ¢ ¢ < tn <tn+1 = t. In the present paper, using simple formulas for the conditional expectations with the conditioning functions Xn and Xn+1, we evaluate the Lp(1 · p · 1)-analytic conditional Fourier-Feynman transforms and the conditional convolution products of the functions which have the form Z L2[0;t] expfi(v; x)gd¾(v) ZRr exp ½i Xrj=1zj(vj ; x)¾d½(z1; ¢ ¢ ¢ ; zr) for x 2 C[0; t], where fv1; ¢ ¢ ¢ ; vrg is an orthonormal subset of L2[0; t] and ¾ and ½ are the complex Borel measures of bounded variations on L2[0; t] and Rr, respectively. We then investigate the inverse transforms of the function with their relationships and¯nally prove that the analytic conditional Fourier-Feynman trans-forms of the conditional convolution products for the functions, can be expressed in terms of the products of the conditional Fourier- Feynman transforms of each function.
1. Introduction and preliminaries
2. Conditional Fourier-Feynman transform with ¯nal time conditioning function
3. Conditional Fourier-Feynman transform without ¯nal time conditioning function
4. Relationships between conditional Fourier-Feynman trans- forms and convolutions
(0)
(0)