Appendix 17.1: Derivation of Ito's Lemma

Let X be a generalized Wiener process whose law of motion is described by:

img

Now, define f(x) as a real valued function of X—for example, f(x) is a derivative of X whose law of motion we wish to determine. Expand f(x) using a Taylor series:

img

Then, in the limit, as img we get:

img

We are recognizing here that this result holds because the higher order terms go to zero faster as Δ approaches zero. This is the fundamental theorem of calculus. But in stochastic calculus, the second order term img does not vanish because X is normally distributed with positive variance, which converges in probability to img. This can be conceptualized from the Wiener process itself, where the term img has variance img, since img.

So, while the fundamental theorem of calculus is:

img

we must extend this to include functions of time (where img) so that for f = f(X,t), we get:

img

Equivalently,

img

because img, since t is deterministic and img vanishes.

This is the simplest form of Ito's lemma. If we have a model for the law of motion for X, then we can derive a model of the law of motion for a derivative of X.

Therefore, taking our generalized Wiener process from before and permitting the parameters μ and σ each to also be functions of X and t, then it follows by definition that:

img

And, substituting for img, dX2 and then dX,

img

Rearranging, we solve for the law of motion for the derivative:

img

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