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(Other variations of Brownian motion). Theorem 3.4.3 asserts that if $T$ is a positive number and we choose a partition $\Pi$ with points $0=t_0<t_1<t_2<\cdots<t_n=T$, then as the number $n$ of partition points approaches infinity and the length of the longest subinterval $\|\Pi\|$ approaches zero, the sample quadratic variation $$ \sum_{j=0}^{n-1}\left(W\left(t_{j+1}\right)-W\left(t_j\right)\right)^2 $$ approaches $T$ for almost every path of the Brownian motion $W$. In Remark 3.4.5, we further showed that $\sum_{j=0}^{n-1}\left(W\left(t_{j+1}\right)-W\left(t_j\right)\right)\left(t_{j+1}-t_j\right)$ and $\sum_{j=0}^{n-1}\left(t_{j+1}-t_j\right)^2$ have limit zero. We summarize these facts by the multiplication rules $$ d W(t) d W(t)=d t, \quad d W(t) d t=0, \quad d t d t=0 . $$

     (Other variations of Brownian motion). Theorem 3.4.3 asserts that if $T$ is a positive number and we choose a partition $\Pi$ with points $0=t_0<t_1<t_2<\cdots<t_n=T$, then as the number $n$ of partition points approaches infinity and the length of the longest subinterval $\|\Pi\|$ approaches zero, the sample quadratic variation
$$
\sum_{j=0}^{n-1}\left(W\left(t_{j+1}\right)-W\left(t_j\right)\right)^2
$$
approaches $T$ for almost every path of the Brownian motion $W$. In Remark 3.4.5, we further showed that $\sum_{j=0}^{n-1}\left(W\left(t_{j+1}\right)-W\left(t_j\right)\right)\left(t_{j+1}-t_j\right)$ and $\sum_{j=0}^{n-1}\left(t_{j+1}-t_j\right)^2$ have limit zero. We summarize these facts by the multiplication rules
$$
d W(t) d W(t)=d t, \quad d W(t) d t=0, \quad d t d t=0 .
$$
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Stochastic Calculus for Finance II : Continuous-Time Models
Stochastic Calculus for Finance II : Continuous-Time Models
Steven E. Shreve 1st Edition
Chapter 3, Problem 4 ↓

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- $W(t)$ represents a Brownian motion, which is a continuous-time stochastic process with independent and normally distributed increments. - A partition $\Pi$ of the interval $[0, T]$ is given by $0 = t_0 < t_1 < t_2 < \cdots < t_n = T$. - $\|\Pi\|$ denotes the  Show more…

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(Other variations of Brownian motion). Theorem 3.4.3 asserts that if $T$ is a positive number and we choose a partition $\Pi$ with points $0=t_0<t_1<t_2<\cdots<t_n=T$, then as the number $n$ of partition points approaches infinity and the length of the longest subinterval $\|\Pi\|$ approaches zero, the sample quadratic variation $$ \sum_{j=0}^{n-1}\left(W\left(t_{j+1}\right)-W\left(t_j\right)\right)^2 $$ approaches $T$ for almost every path of the Brownian motion $W$. In Remark 3.4.5, we further showed that $\sum_{j=0}^{n-1}\left(W\left(t_{j+1}\right)-W\left(t_j\right)\right)\left(t_{j+1}-t_j\right)$ and $\sum_{j=0}^{n-1}\left(t_{j+1}-t_j\right)^2$ have limit zero. We summarize these facts by the multiplication rules $$ d W(t) d W(t)=d t, \quad d W(t) d t=0, \quad d t d t=0 . $$
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Key Concepts

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Brownian Motion
A Brownian motion is a continuous-time stochastic process with independent, normally distributed increments that model random movement. It serves as a key example of a martingale and is the cornerstone of many developments in stochastic calculus and financial mathematics.
Quadratic Variation
Quadratic variation measures the accumulated squared increments of a process over a time interval. For Brownian motion, its quadratic variation over an interval [0, T] is equal to T, demonstrating a unique path property that distinguishes it from processes with smooth paths.
Itô Calculus
Itô calculus is a branch of mathematics that extends traditional calculus to stochastic processes. The multiplication rules, such as dW(t)dW(t) = dt, dW(t)dt = 0, and dt dt = 0, formalize the manipulation of differentials in this context, reflecting the fact that increments of Brownian motion have non-trivial quadratic variation while their first-order terms vanish.
Partitioning and Limit Processes
Partitioning an interval into smaller subintervals and then taking the limit as the mesh size approaches zero is a critical technique in defining integrals and variations. This approach underpins the rigorous derivation of properties such as the quadratic variation of Brownian motion and the resulting differential rules in stochastic calculus.

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(Hitting Times for Brownian Motion) Let W(t) be a standard Brownian motion. Let a > 0 and define Ta as the first time that W(t) = a. That is, Ta = min{t : W(t) = a}. a. Show that for any t ≥ 0, we have P(W(t) ≥ a) = P(W(t) ≥ a | Ta ≤ t)P(Ta ≤ t). b. Using Part (a), show that P(Ta ≤ t) = 2 [1 - Φ(a/∙t)]. c. Using Part (b), show that the PDF of Ta is given by f_{Ta}(t) = (a / (t√(2πt))) * exp(-a^2 / (2t)). Note: By symmetry of Brownian motion, we conclude that for any a ≠ 0, we have f_{Ta}(t) = (|a| / (t√(2πt))) * exp(-a^2 / (2t)).

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