CONTENTS

Exercise: Girsanov Failure — Novikov Condition Violation

Prerequisites: Girsanov's Theorem

Problem

Novikov's condition — EP[exp(120Tθs2ds)]<\mathbb{E}^{\mathbb{P}}[\exp(\tfrac{1}{2}\int_0^T\theta_s^2\,ds)] < \infty — is sufficient for the Doléans-Dade exponential ZtZ_t to be a true martingale (not merely a local martingale). When Novikov fails, ZtZ_t can still be a strict local martingale with E[ZT]<1\mathbb{E}[Z_T] < 1, and then the proposed measure Q\mathbb{Q} from Girsanov is a sub-probability measure — not a valid probability measure.
  1. Consider a fixed horizon TT and suppose θt=αWt\theta_t = \alpha\cdot W_t for some α>0\alpha > 0, where WtW_t is a P\mathbb{P}-BM. Check whether Novikov's condition holds. (Hint: compute 0TWs2ds\int_0^T W_s^2\,ds's distribution; you will find that E[exp(α220TWs2ds)]\mathbb{E}[\exp(\tfrac{\alpha^2}{2}\int_0^T W_s^2\,ds)] is an integral of an unbounded exponential against a gaussian — check whether it is finite.)

  2. For what values of αT\alpha T does EP[exp(α220TWs2ds)]=\mathbb{E}^{\mathbb{P}}[\exp(\tfrac{\alpha^2}{2}\int_0^T W_s^2\,ds)] = \infty? Use the fact that 0TWs2ds\int_0^T W_s^2\,ds has a known distribution related to chi-squared.

  3. When Novikov fails, can we use a weaker sufficient condition (Kazamaki: E[exp(12θdW)]<\mathbb{E}[\exp(\tfrac{1}{2}\int \theta\,dW)] < \infty) to rescue the argument? Explain qualitatively.

  4. Practical implication. In the Heston stochastic-volatility model dvt=κ(θvvt)dt+ξvtdWtvdv_t = \kappa(\theta_v - v_t)\,dt + \xi\sqrt{v_t}\,dW^v_t, certain parameter combinations can violate Novikov — the martingale measure is not well-defined on all horizons. What does this mean for using Heston for long-dated-options pricing? Would you blindly trust the Q\mathbb{Q} prices?

Hint

Part 1's integral 0TWs2ds\int_0^T W_s^2\,ds has mean T2/2T^2/2 and a distribution that, via the Cameron-Martin-like expansion, relates to the quadratic functional of Brownian motion. The key question is whether the MGF of this integral is finite at α2/2\alpha^2/2.

Jump to the solution when you're ready.