TheoremComplete

Signed Measures and Radon-Nikodym - Applications

TheoremConditional Expectation via Radon-Nikodym

Let (Ω,F,P)(\Omega, \mathcal{F}, \mathbb{P}) be a probability space and XX be an integrable random variable (XL1(P)X \in L^1(\mathbb{P})). Let GF\mathcal{G} \subseteq \mathcal{F} be a sub-sigma-algebra.

Define a signed measure ν\nu on (Ω,G)(\Omega, \mathcal{G}) by: ν(A)=AXdP for AG\nu(A) = \int_A X \, d\mathbb{P} \text{ for } A \in \mathcal{G}

Then νPG\nu \ll \mathbb{P}|_{\mathcal{G}}, and by Radon-Nikodym, there exists a G\mathcal{G}-measurable function YY such that: ν(A)=AYdP for all AG\nu(A) = \int_A Y \, d\mathbb{P} \text{ for all } A \in \mathcal{G}

This function YY is the conditional expectation of XX given G\mathcal{G}, denoted E[XG]\mathbb{E}[X | \mathcal{G}].

This theorem shows that conditional expectation is essentially the Radon-Nikodym derivative, providing a rigorous foundation for conditional probability and expectation in probability theory.

ExampleComputing Conditional Expectations

Let XX and YY be jointly distributed random variables on R2\mathbb{R}^2 with joint density fX,Y(x,y)f_{X,Y}(x, y).

The conditional expectation E[YX=x]\mathbb{E}[Y | X = x] can be computed via Radon-Nikodym. Define: ν(A)=AyfX,Y(x,y)dy\nu(A) = \int_A y f_{X,Y}(x, y) \, dy

The marginal density of XX is fX(x)=fX,Y(x,y)dyf_X(x) = \int f_{X,Y}(x, y) \, dy. By Radon-Nikodym: E[YX=x]=dνdfX(x)=yfX,Y(x,y)dyfX(x)\mathbb{E}[Y | X = x] = \frac{d\nu}{d f_X}(x) = \frac{\int y f_{X,Y}(x, y) \, dy}{f_X(x)}

This is the familiar formula for conditional expectation in terms of densities.

Remark

Applications of Radon-Nikodym in various fields:

  1. Likelihood ratios: In statistics, the likelihood ratio between two probability measures P\mathbb{P} and Q\mathbb{Q} (with QP\mathbb{Q} \ll \mathbb{P}) is: L=dQdPL = \frac{d\mathbb{Q}}{d\mathbb{P}}

This is fundamental for hypothesis testing and Bayesian inference.

  1. Girsanov's theorem: In stochastic calculus, changing probability measures (to eliminate drift in SDEs) uses Radon-Nikodym derivatives: dQdP=exp(0TθsdWs120Tθs2ds)\frac{d\mathbb{Q}}{d\mathbb{P}} = \exp\left(\int_0^T \theta_s \, dW_s - \frac{1}{2}\int_0^T \theta_s^2 \, ds\right)

  2. Martingale theory: Martingales can be characterized via Radon-Nikodym derivatives of conditional distributions.

  3. Information theory: The Kullback-Leibler divergence between measures involves the Radon-Nikodym derivative: DKL(QP)=log(dQdP)dQD_{KL}(\mathbb{Q} || \mathbb{P}) = \int \log\left(\frac{d\mathbb{Q}}{d\mathbb{P}}\right) d\mathbb{Q}

  4. Optimal stopping: The value function in optimal stopping problems can be expressed using Radon-Nikodym derivatives of stopped processes.

The Radon-Nikodym theorem's applications span probability, statistics, finance, and physics, making it one of the most practically important results in measure theory.