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Deriving Shreve’s Girsanov Result with Quadratic Covariation

Article Quant Q&A · Author: athos

Summary

The document explains how a one-dimensional version of Girsanov’s theorem in Shreve’s stochastic calculus text follows from a more general formulation. The key identification is to take the Brownian motion as the local martingale and use the negative stochastic integral of the adapted drift process against Brownian motion as the change-of-measure process. The resulting density is the stochastic exponential appearing in Shreve’s statement.

The derivation hinges on the covariation identity between Brownian motion and its stochastic integral: their quadratic covariation is the integral of the integrand against Brownian quadratic variation, with the negative sign inherited from the chosen process. Since Brownian motion has quadratic variation equal to elapsed time, the correction term becomes the time integral of the drift. The discussion is a concise calculation rather than a full proof; it relies on standard stochastic calculus rules and does not address the integrability condition needed for the change of measure.

Key ideas

  • Shreve’s theorem is obtained as a special case of the more general Girsanov formulation.
  • Choose the change-of-measure process as the negative stochastic integral of the adapted drift against Brownian motion.
  • The covariation of Brownian motion with that stochastic integral equals the negative integral of the drift over time.
  • The identity follows from Brownian motion’s quadratic variation being elapsed time.
  • The calculation alone does not establish the integrability condition required for the measure change.

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# Girsanov Theorem and Quadratic Variation


# Girsanov Theorem and Quadratic Variation












Girsanov theorem seems to have many different forms. I've got a problem matching the form in wiki to the one in Shreve's book, due to the difficulty of quadratic variation calculation.

Below is the Girsanov Theorem from wiki:

> Let $\{W_t\}$ be a Wiener process on the Wiener probability space $\{\Omega,\mathcal{F},P\}$. Let $X_t$ be a measurable process adapted to the natural filtration of the Wiener process $\{\mathcal{F}^W_t\}$. Given an adapted process $X_t$ with $X_0 = 0$, define $Z_t=\mathcal{E}(X)_t,\,$ where $\mathcal{E}(X)$ is the stochastic exponential (or Doléans exponential) of X with respect to W, i.e. $\mathcal{E}(X)_t=\exp \left ( X_t - \frac{1}{2} [X]_t \right )$, where $[X]_t$ is a quadratic variation for $X_t$. Thus $Z_t$ is a strictly positive local martingale, and a probability measure $Q$ can be defined on $\{\Omega,\mathcal{F}\}$ such that we have Radon–Nikodym derivative $\frac{d Q}{d P} |_{\mathcal{F}_t} = Z_t = \mathcal{E} (X)_t$. Then for each $t$ the measure $Q$ restricted to the unaugmented sigma fields $\mathcal{F}^W_t$ is equivalent to $P$ restricted to $\mathcal{F}^W_t.\,$ Furthermore if $Y$ is a local martingale under $P$ then the process $\tilde Y_t = Y_t - \left[ Y,X \right]_t$ is a $Q$ local martingale on the filtered probability space $\{\Omega,F,Q,\{F^W_t\}\}$.

Below is the Girsanov Theorem from Shreve's book "Stochastic calculus for finance II"

> Theorem 5.2.3 (Girsanov, one dimension). Let $W(t)$, $0 \leq t \leq T$, be a Brownian motion on a probability space $(\Omega, \mathscr F, \mathbb P)$, and let $\mathscr F(t)$, $0 \leq t \leq T$, be a filtration for this Brownian motion. Let $\Theta(t)$, $0 \leq t \leq T$, be an adapted process. Define $$Z(t) = \text{exp} \left\{ -\int_0^t \Theta(u)dW(u) - \frac{1}{2} \int_0^t \Theta^2(u) du \right \}, \tag{5.2.11}$$ $$\widetilde W(t) = W(t) + \int_0^t \Theta(u) du, \tag{5.2.12}$$ and assume that $$\mathbb E \int_0^T \Theta^2(u) Z^2(u) du < \infty \tag{5.2.13}$$ Set $Z = Z(T)$. Then $\mathbb E Z = 1$ and under the probability measure $\widetilde P$ given by (5.2.1), the process $\widetilde W(t)$, $0 \leq t \leq T$, is a Brownian motion.

Seems the Girsanov theorem form wiki is more general than the one on Shreve's book.

Now my questions is: How to derive the latter from the former?

It seems only need to take $Y(t) = W(t)$ and $X(t) = \int_0^t \Theta(u) du$ in the wiki definition. This left to prove

$$[W(t), \int_0^t \Theta(u) du]_t = - \int_0^t \Theta(u) du$$

, but how to calculate the quadratic variation?

Quadratic variation definition is $$[X,Y](T) := \lim_{\|\Pi\|\to 0} \sum_{j=0}^{n-1} \left[ X(t_{j+1}) - X(t_j) \right] \left[ Y(t_{j+1}) - Y(t_j) \right]$$ , where $\Pi := \{ t_0, t_1, \cdots, t_n \}$ . But I'm a bit stuck here.

Could you please kindly give me some hint how to proceed?

## Answer by emcor (score 11, accepted)

https://quant.stackexchange.com/a/14795

Shreve's theorem also called "Girsanov II" indeed represents a special case of the general "Girsanov I" from Wiki above, with $$Y_t:=W_t,$$$$X_t:=-\int_0^t\Theta_udW_u$$

We can show: $$[Y,X]=-\int_0^t\Theta_udu$$ by using general Stochastic Calculus rules (e.g. p.37, 6.6 here):

$$[Y,X]=[W_t,-\int_0^t\Theta_udW_u]=-\int_0^t\Theta_ud[W_u,W_u]=-\int_0^t\Theta_udu$$

as $[W,W]=[W]=t$.

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.