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

Diffusions, SDEs, and the Feynman-Kac Formula — Overview

Itô's formula takes a process and tells you how smooth functions of it evolve. The natural next question is the inverse: given a desired dynamics dXt=b(t,Xt) dt+σ(t,Xt) dWtdX_t = b(t, X_t) \, dt + \sigma(t, X_t) \, dW_t, does such a process exist? The answer — yes, under Lipschitz conditions, by Picard iteration — is the existence-uniqueness theorem for SDEs, and the process is called a diffusion.
The payoff of solving an SDE is the Feynman-Kac formula: a deep connection between diffusions and PDEs. Specifically, the solution u(t,x)=E[g(XT)e−∫tTc(Xs)ds∣Xt=x]u(t, x) = \mathbb{E}[g(X_T) e^{-\int_t^T c(X_s)ds} | X_t = x] to a terminal-value problem satisfies a parabolic PDE — and conversely, the solution to the PDE can be represented as such an expectation. In finance, this is the link between option pricing (an expectation under Q\mathbb{Q}) and the Black-Scholes PDE (a parabolic equation for the option price). These are not two separate methods; they are two faces of the same object.

In this lesson

  1. Contents
  2. Three logical layers
  3. Finance reading
  4. Connections

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