Consider the Ornstein-Uhlenbeck process, $U(t)$, whose evolution follows: $$ \mathrm{d}U(t) = -\theta U(t) \mathrm{d}t + \sigma \mathrm{d}W(t), $$ where $\theta \in (0,2)$ is the mean-reversion rate, $\sigma >0$ is the dispersion rate, and $\{W(t)|t\geq0\}$ is a standard Brownian motion. Note that this is a zero-mean OU process. Now consider a new variable, $V(t)$, which is a function of $U(t)$ and a geometric Brownian motion, $X(t)$: $$ V(t) = \ln{\left[\frac{X(t) + U(t)}{X(t)}\right]}, $$ where $\{X(t),X(t)+U(t)>0|t\geq0\}$, and $X(t)$ follows: $$ \mathrm{d}X(t) = \mu X(t) \mathrm{d}t + \eta X(t) \mathrm{d}Z(t), $$ where $\mu, \eta >0$ are the drift and dispersion rates, respectively, and $\{Z(t)|t\geq0\}$ is a standard Brownian motion independent of $W(t)$ for all time.
Is it possible to show that $U(t)$ and $V(t)$ are perfectly positively correlated? Or, more importantly, is it possible to determine the conditions under which they are perfectly positively correlated? Simulations have shown me that the two are almost perfectly correlated, but I lack a formal proof.