  In this paper an analytic operator-valued generalized Feynman integral was
studied on a very general Wiener space $C_{a,b}[0,T]$. The general Wiener space
$C_{a,b}[0,T]$ is a function space which is induced by the generalized Brownian
motion process associated with continuous functions $a$ and $b$. The structure
of the analytic operator-valued generalized Feynman integral is suggested and
the existence of the analytic operator-valued generalized Feynman integral is
investigated as an operator from $L^1(\mathbb R, \nu_{\delta,a})$ to
$L^{\infty}(\mathbb R)$ where $\nu_{\delta,a}$ is a $\sigma$-finite measure on
$\mathbb R$ given by \[ d\nu_{\delta,a}=\exp\{\delta \mathrm{Var}(a)u^2\} du,
\] where $\delta>0$ and $\mathrm{Var}(a)$ denotes the total variation of the
mean function $a$ of the generalized Brownian motion process. It turns out in
this paper that the analytic operator-valued generalized Feynman integrals of
functionals defined by the stochastic Fourier--Stieltjes transform of complex
measures on the infinite dimensional Hilbert space $C_{a,b}'[0,T]$ are elements
of the linear space \[ \bigcap_{\delta>0} \mathcal L( L^1(\mathbb
R,\nu_{\delta,a}),L^{\infty}(\mathbb R)). \]
