CONTENTS

Exercise: Reading Moments from the MGF — Normal Distribution

Problem

Let XN(0,σ2)X \sim \mathcal{N}(0, \sigma^2).

  1. State MX(s)M_X(s). Write it as a Taylor series in ss up to order s8s^8.

  2. By reading off Taylor coefficients, derive the formula E[X2k]=(2k1)!!σ2k,E[X2k+1]=0,\mathbb{E}[X^{2k}] = (2k - 1)!!\cdot \sigma^{2k}, \qquad \mathbb{E}[X^{2k+1}] = 0, for k=0,1,2,3,4k = 0, 1, 2, 3, 4. Verify (2k1)!!=1,1,3,15,105,(2k - 1)!! = 1, 1, 3, 15, 105, \ldots (the double factorial of odd numbers).

  3. Kurtosis of the normal. Recall excess kurtosis is E[X4]/σ43\mathbb{E}[X^4]/\sigma^4 - 3. Verify this is 00 for the normal — the definitional fact that "normal has zero excess kurtosis."
  4. Black-Scholes application. For WTN(0,T)W_T \sim \mathcal{N}(0, T), compute E[WT4]\mathbb{E}[W_T^4] as a function of TT. Explain why this appears in the variance of integrated Brownian motion 0TWt2dt\int_0^T W_t^2\,dt (see the quadratic variation discussion in the Itô's lemma lesson).

Hint

For part 1, MX(s)=exp(σ2s2/2)M_X(s) = \exp(\sigma^2 s^2/2), and exp(u)=1+u+u2/2!+u3/3!+u4/4!+\exp(u) = 1 + u + u^2/2! + u^3/3! + u^4/4! + \ldots with u=σ2s2/2u = \sigma^2 s^2/2. Collect powers of ss.

Jump to the solution when you're ready.