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Stochastic Calculus / Diffusions, SDEs, and the Feynman-Kac Formula

Stochastic Differential Equations: Strong and Weak Solutions

Every financial model that involves randomness specifies an SDE. But writing dSt=μSt dt+σSt dWtdS_t = \mu S_t \, dt + \sigma S_t \, dW_t is only meaningful if a process StS_t satisfying this equation actually exists. The question "does there exist a solution?" is non-trivial: some SDEs have no solution, some have infinitely many, and some have a unique solution that exists only up to a random time.

The answer for the models used in finance is reassuring: under a Lipschitz condition on the drift b(t,x)b(t,x) and diffusion σ(t,x)\sigma(t,x) coefficients plus a linear growth condition, the SDE dXt=b(t,Xt) dt+σ(t,Xt) dWtdX_t = b(t, X_t) \, dt + \sigma(t, X_t) \, dW_t has a unique strong solution for all time. The Picard iteration that proves this in the deterministic setting extends verbatim to the stochastic case, with L2L^2 norm replacing the supremum norm.
This note also contrasts strong solutions (built on a given Brownian motion) with weak solutions (where the probability space and BM are part of the solution), and explains why the distinction matters for simulation: when a strong solution exists, you can simulate XtX_t by simulating WtW_t and applying a deterministic functional.
Learning objectives. By the end of this note you should be able to:
  • State the definition of a strong solution to an SDE and explain the "causality" requirement.
  • State and apply the existence-uniqueness theorem (Itô's theorem) under Lipschitz and linear growth.
  • Verify that GBM and the OU/Vasicek process satisfy the Lipschitz condition.
  • Distinguish strong solutions from weak solutions and give a canonical example of each.
  • Apply Picard iteration to estimate the L2L^2 error of successive approximations.

In this lesson

  1. Setting and Definitions
  2. The Existence-Uniqueness Theorem
  3. Key Examples
  4. Weak Solutions
  5. Simulation Consequence: Strong Solutions

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