The integrand is a bounded previsible process, so is a continuous local martingale. The quadratic variation of a stochastic integral isbecause the Brownian zero set has zero Lebesgue measure. Since , the Lévy characterization of Brownian motion shows that is a standard Brownian motion.
Both variables are centered. The Itô isometry in its bilinear form giveswhere the last equality follows because a centered Gaussian distribution is a symmetric probability distribution. Thus and are uncorrelated random variables.
They are not independent. The Itô formula gives , and the bilinear Itô isometry therefore givesIf and were independent random variables, then would also be independent of the measurable function , and centeredness would instead give . This contradiction disproves independence.
The Dambis-Dubins-Schwarz theorem states that if is a continuous local martingale with and , then, forthe process is a standard Brownian motion and . If , one obtains the same representation after enlarging the probability space and continuing independently beyond .
Set . Its quadratic variation is , which is continuous and tends to infinity almost surely by assumption. The stated stopping time is the inverse clock at level one, so . The Dambis-Dubins-Schwarz theorem gives
The assertion is false: the Brownian motion produced by the Dambis-Dubins-Schwarz theorem need not be independent of its clock. Let be a standard Brownian motion and setIf the Brownian motion in were independent of the whole quadratic variation process, then conditioning on would give . Instead, the fourth-moment formula for a bivariate normal distribution gives for , and henceThus and are dependent.
Because independent Brownian motions have zero quadratic covariation, the Itô product rule givesAfter integration, the random variable in the question is . Writing for independent standard Gaussian random variables , its distribution isthe scaled product of two independent standard normal random variables.
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