CONTENTS

Solution: Apply Itô — d(eWt)d(e^{W_t}) and E[eWt]\mathbb{E}[e^{W_t}]

Part 1

With V(W)=eWV(W) = e^W, dXt=dWtdX_t = dW_t (so a=0a = 0, b=1b = 1), and V=V=eWV' = V'' = e^W:

dYt=(0+0eWt+1212eWt)dt+1eWtdWt=12eWtdt+eWtdWtdY_t = \left(0 + 0\cdot e^{W_t} + \tfrac{1}{2}\cdot 1^2\cdot e^{W_t}\right)dt + 1\cdot e^{W_t}\,dW_t = \tfrac{1}{2}e^{W_t}\,dt + e^{W_t}\,dW_t
Or equivalently dYt=12Ytdt+YtdWtdY_t = \tfrac{1}{2}Y_t\,dt + Y_t\,dW_t. The drift is 12Yt\tfrac{1}{2}Y_t and the diffusion is YtY_t. The 12Ytdt\tfrac{1}{2}Y_t\,dt is the Itô correction — under ordinary calculus we would get only dYt=YtdWtdY_t = Y_t\,dW_t and miss the drift entirely.

Part 2

Taking expectations and using that 0teWsdWs\int_0^t e^{W_s}\,dW_s is a mean-zero martingale (under the usual integrability assumption, which holds because E[0Te2Wsds]<\mathbb{E}[\int_0^T e^{2W_s}\,ds] < \infty):

dmdt=12m(t),m(0)=1\frac{dm}{dt} = \tfrac{1}{2}m(t), \quad m(0) = 1

Solution: m(t)=et/2m(t) = e^{t/2}.

Part 3

WtN(0,t)W_t \sim \mathcal{N}(0, t) has moment-generating function E[eλWt]=eλ2t/2\mathbb{E}[e^{\lambda W_t}] = e^{\lambda^2 t / 2}. With λ=1\lambda = 1:

E[eWt]=et/2\mathbb{E}[e^{W_t}] = e^{t/2}

This matches part 2 exactly. Two routes, one answer — the Itô-calculus route is longer here but generalises to V(Wt)V(W_t) for any smooth VV, whereas the direct route requires knowing the distribution in closed form.

Part 4

Yt=eWtY_t = e^{W_t} is not a martingale: its drift 12Ytdt\tfrac{1}{2}Y_t\,dt is strictly positive, and E[Yt]=et/2\mathbb{E}[Y_t] = e^{t/2} grows exponentially.

To cancel the drift, set Y~t=eαWt+βt\tilde Y_t = e^{\alpha W_t + \beta t} and apply Itô to V(t,W)=eαW+βtV(t, W) = e^{\alpha W + \beta t}:

  • Vt=βVV_t = \beta V
  • VW=αVV_W = \alpha V
  • VWW=α2VV_{WW} = \alpha^2 V

Itô gives dY~t=(β+12α2)Y~tdt+αY~tdWtd\tilde Y_t = (\beta + \tfrac{1}{2}\alpha^2)\tilde Y_t\,dt + \alpha\tilde Y_t\,dW_t. The drift vanishes iff β=12α2\beta = -\tfrac{1}{2}\alpha^2. So the martingale correction is:

Y~t=exp ⁣(αWt12α2t)\tilde Y_t = \exp\!\left(\alpha W_t - \tfrac{1}{2}\alpha^2 t\right)
This is the Doléans-Dade exponential — the cornerstone of Girsanov's theorem. The 12α2t-\tfrac{1}{2}\alpha^2 t is exactly the Itô correction: it offsets the +12α2+\tfrac{1}{2}\alpha^2 that Itô's lemma introduces.

Takeaways

  • The Itô correction for eWte^{W_t} adds a 12\tfrac{1}{2} drift — the same 12\tfrac{1}{2} that appears in the log-normal moment formula.
  • Two routes to the same expectation. Itô + ODE is the constructive route; the Gaussian MGF is the direct route. Quant finance uses both routinely.
  • To make an exponential a martingale, subtract half its variance-accumulation. This single identity (E[eαWtα2t/2]=1\mathbb{E}[e^{\alpha W_t - \alpha^2 t/2}] = 1) drives the Doléans-Dade exponential, change-of-measure arguments, and the 12σ2-\tfrac{1}{2}\sigma^2 term in log-GBM.