Brownian Motion and Stochastic Calculus: Moments, Integrals, and Itô’s Formula
Summary
This note collects basic properties of deterministic functions, Brownian motion, and processes driven by Brownian motion. It lists derivatives, integrals, expectations, and variances, and introduces the idea that Brownian paths are not differentiable in the ordinary sense. It also gives Brownian moment formulas and a version of Itô’s formula, which adds a second-derivative term when a function is applied to Brownian motion.
The table is a rough reference rather than a reliable derivation: several entries are incomplete or incorrect, including integrals involving Brownian motion and the stated process definitions. The note does not provide assumptions, proofs, or worked examples to resolve these issues. Readers can take away the distinction between ordinary and stochastic calculus, but should verify formulas against a sound stochastic calculus reference before using them in quantitative models.
Key ideas
- Brownian motion has no ordinary time derivative because its paths are not smooth.
- Brownian motion at time t has mean zero and variance t.
- Odd moments of a centered Gaussian variable vanish, while even moments follow a double-factorial formula.
- Itô’s formula includes a second-derivative correction for functions of Brownian motion.
- The table contains errors and should not be used as a formula reference without checking.
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# Summary of Stochastic Derivatives, Integrals, Expectations, and Variances
# Summary of Stochastic Derivatives, Integrals, Expectations, and Variances
I wanted to make a summary table of stochastic functions to improve my understanding. Maybe the following should be a wiki page on this site so others can add functions and examples? Does the following look right?
Let,
$c$ be a constant $k$ be a natural number $t$ be a variable representing time $f(t)$ be a deterministic function of time $t$ $B_t$ be Brownian motion $X_t$ be a random process driven by $B_t$ in some way
| Function | Derivative | Integral | Expectation | Variance |
| $f(t)$ | $\frac{d}{dt}f(t)=f'(t)$ | $\int_0^t f(s)dB_s=X_t$ | $\mathbb{E}[f(t)]=f(t)$ | $\mbox{Var}[f(t)]=0$ |
| $B_t$ | $\frac{d}{dt} B_t=\mbox{undefined}$ | $\int_0^t B_s ds=\frac{1}{2}B_t^2 - \frac{1}{2}tB_t$ $\int_0^t B_s dB_s=\frac{1}{2}B_t^2-\frac{1}{2}t$ | $\mathbb{E}[B_t]=0$ | $\mbox{Var}[B_t]=t$ |
| $cB_t$ | $\frac{d}{dt} cB_t=\mbox{undefined}$ | $\int_0^t cB_s ds=ctB_t$ $\int_0^t B_s dB_s=c(\frac{1}{2}B_t^2-\frac{1}{2})t$ | $\mathbb{E}[cB_t]=0$ | $\mbox{Var}[cB_t]=c^2t$ |
| $tB_t$ | $\frac{d}{dt} tB_t =B_t$ | $\int_0^t tB_s ds=\frac{t^2}{2}B_t$ $\int_0^t B_s dB_s=\frac{1}{2}B_t^2 t-\frac{1}{2}t^2$ | $\mathbb{E}[tB_t]=0$ | $\mbox{Var}[tB_t]=t^2 \cdot t$ |
| $B^2_t$ | $\frac{d}{dt} B^2_t=\mbox{undefined}$ | $\int_0^t B^2_tds=?$ $\int_0^t B^2_t dB_t = \frac{1}{3} B^3_t-tB_t$ | $\mathbb{E}[B^2_t]=t $ | $\mbox{Var}[B_t^2]=t^2$ |
| $B^k_t$ | $\frac{d}{dt} B^k_t=\mbox{undefined}$ | - | $\mathbb{E}[B_t^{2k}]=t^k(2k-1)!!$ See note 1 | - |
| $X_t = x + \mu dt+\sigma B_t$ | $dX_t = a_tdt+b_tdB_t$ | $\int_0^t X_s ds = t X_s$ $\int_0^t X_s dX_s = \frac{1}{2}X^2_s - \frac{1}{2}t$ | - | - |
| $f(B_t) = f(0) + \frac{1}{2} \int_0^t f''(B_s)ds + \int_0^t f'(B_s)ds$ | $df(B_t) = f'(B_t)dB_t + \frac{1}{2} f''(B_t)dt$ | - | - | - |
Note 1 - All odd moments are 0. $(2k-1)!!$ is the product of all odd integers between 1 and $2k-1$.
Note that $\frac{d}{dt} (B_t)$ is undefined because $B_t$ is non-smooth.
Note that taking the derivative with respect to Brownian motion $\frac{d}{dB_t}$ is undefined because $B_t$ is a function. This would be similar to taking the derivative with respect to another function $f(\cdot)$ such as $\frac{d}{df}$ which doesn't make sense.Shown in full with attribution under the source's licence. Licence: CC BY-SA 4.0 (Stack Exchange)
This summary was written by Stratmill's research agent from the original; it is not a copy of the source.