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(Decomposition of correlated Brownian motions into independent Brownian motions). Suppose $B_1(t)$ and $B_2(t)$ are Brownian motions and $$ d B_1(t) d B_2(t)=\rho(t) d t $$ 198 4 Stochastic Calculus where $\rho$ is a stochastic process taking values strictly between -1 and 1 . Define processes $W_1(t)$ and $W_2(t)$ such that $$ \begin{aligned} & B_1(t)=W_1(t), \\ & B_2(t)=\int_0^t \rho(s) d W_1(s)+\int_0^t \sqrt{1-\rho^2(s)} d W_2(s), \end{aligned} $$ and show that $W_1(t)$ and $W_2(t)$ are independent Brownian motions.

    (Decomposition of correlated Brownian motions into independent Brownian motions). Suppose $B_1(t)$ and $B_2(t)$ are Brownian motions and
$$
d B_1(t) d B_2(t)=\rho(t) d t
$$
198
4 Stochastic Calculus
where $\rho$ is a stochastic process taking values strictly between -1 and 1 . Define processes $W_1(t)$ and $W_2(t)$ such that
$$
\begin{aligned}
& B_1(t)=W_1(t), \\
& B_2(t)=\int_0^t \rho(s) d W_1(s)+\int_0^t \sqrt{1-\rho^2(s)} d W_2(s),
\end{aligned}
$$
and show that $W_1(t)$ and $W_2(t)$ are independent Brownian motions.
Show more…
Stochastic Calculus for Finance II : Continuous-Time Models
Stochastic Calculus for Finance II : Continuous-Time Models
Steven E. Shreve 1st Edition
Chapter 4, Problem 13 ↓

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Step 1: **Define the processes $W_1(t)$ and $W_2(t)$** Given the definitions: \[ B_1(t) = W_1(t) \] \[ B_2(t) = \int_0^t \rho(s) dW_1(s) + \int_0^t \sqrt{1-\rho^2(s)} dW_2(s) \]  Show more…

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(Decomposition of correlated Brownian motions into independent Brownian motions). Suppose $B_1(t)$ and $B_2(t)$ are Brownian motions and $$ d B_1(t) d B_2(t)=\rho(t) d t $$ 198 4 Stochastic Calculus where $\rho$ is a stochastic process taking values strictly between -1 and 1 . Define processes $W_1(t)$ and $W_2(t)$ such that $$ \begin{aligned} & B_1(t)=W_1(t), \\ & B_2(t)=\int_0^t \rho(s) d W_1(s)+\int_0^t \sqrt{1-\rho^2(s)} d W_2(s), \end{aligned} $$ and show that $W_1(t)$ and $W_2(t)$ are independent Brownian motions.
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Key Concepts

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Brownian Motion
A Brownian motion is a continuous-time stochastic process characterized by its continuous paths, stationary and independent increments, and normally distributed changes over time. It serves as the mathematical model for random movement and is central to the theory of stochastic processes and finance.
Correlation Structure
The correlation structure pertains to how two stochastic processes, such as Brownian motions, interact or co-vary over time. In this context, the differential dB?(t)dB?(t) equals ?(t)dt, meaning that the instantaneous covariance between the two processes is governed by the stochastic process ?(t), which lies within (-1, 1). This structure is crucial for understanding how to decompose the processes into independent components.
Decomposition into Independent Components
Decomposing correlated processes into independent components involves representing a correlated Brownian motion as a sum (or integral) of terms involving independent Brownian motions. This is often achieved by using a transformation similar in spirit to the Cholesky decomposition of a covariance matrix, allowing one to express one correlated process as a linear combination of another correlated process and an independent noise term. This decomposition simplifies analysis and is important in fields such as mathematical finance and stochastic modeling.
Stochastic Integration
Stochastic integration is the framework that allows integration with respect to stochastic processes like Brownian motion. It underpins the construction of the decomposed processes, ensuring that the integrals of deterministic or stochastic functions with respect to independent Brownian motions preserve key properties such as being a Brownian motion. This is illustrated by the integrals involving ?(s) and ?(1??²(s)) in the decomposition, where ItÓ calculus guarantees that the resulting processes have the correct distributional and independence properties.

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