Stochastic Calculus

Lesson 6 of 11

Itô's Lemma, Part 2: Product Rule and Isometry

Multiply two random processes and the product rule picks up an extra dX·dY term; square an Itô integral and the isometry turns its variance into an ordinary dt integral.

The product rule gets a third term

In ordinary calculus d(xy)=x dy+y dxd(xy) = x\,dy + y\,dx. The piece you throw away is dx dydx\,dy, a product of two small changes, which is second order. For random processes that piece can be the same size as dtdt, so it stays:

d(XtYt)=Xt dYt+Yt dXt+dXt dYt.d(X_tY_t) = X_t\,dY_t + Y_t\,dX_t + dX_t\,dY_t.

You get it by expanding (X+dX)(Y+dY)−XY(X + dX)(Y + dY) - XY, keeping every term, and simplifying dX dYdX\,dY with the box rules from the Quadratic Variation lesson. The only new rule covers two Brownian motions WW and BB with correlation ρ\rho: dW dB=ρ dtdW\,dB = \rho\,dt. The term dX dYdX\,dY is the cross-variation of XX and YY. Setting Y=XY = X gives d(X2)=2X dX+(dX)2d(X^2) = 2X\,dX + (dX)^2, which is Itô's lemma for f(x)=x2f(x) = x^2, so the two rules agree.

If one factor is smooth, the extra term drops out: d(tWt)=Wt dt+t dWtd(tW_t) = W_t\,dt + t\,dW_t, because dt dW=0dt\,dW = 0. If both factors are Brownian, it survives:

d(WtBt)=Wt dBt+Bt dWt+ρ dt.d(W_tB_t) = W_t\,dB_t + B_t\,dW_t + \rho\,dt.

The two dWdW-type terms have mean zero, so E[WtBt]=ρtE[W_tB_t] = \rho t. With ρ=0.5\rho = 0.5 and t=2t = 2 that is 11, which matches Cov(Wt,Bt)=ρt\mathrm{Cov}(W_t, B_t) = \rho t computed directly. With ρ=0\rho = 0 the rule collapses to the ordinary one and WtBtW_tB_t is a martingale.