TheoremComplete

Signed Measures and Radon-Nikodym - Main Theorem

TheoremLebesgue Decomposition Theorem

Let μ\mu and ν\nu be σ\sigma-finite measures on a measurable space (X,F)(X, \mathcal{F}). Then there exists a unique decomposition: ν=νac+νs\nu = \nu_{ac} + \nu_s

where:

  1. νacμ\nu_{ac} \ll \mu (absolutely continuous with respect to μ\mu)
  2. νsμ\nu_s \perp \mu (mutually singular with μ\mu)

By the Radon-Nikodym theorem, there exists f0f \geq 0 such that: νac(A)=Afdμ for all AF\nu_{ac}(A) = \int_A f \, d\mu \text{ for all } A \in \mathcal{F}

The decomposition ν=νac+νs\nu = \nu_{ac} + \nu_s is unique in the sense that if ν=ν1+ν2\nu = \nu_1 + \nu_2 with ν1μ\nu_1 \ll \mu and ν2μ\nu_2 \perp \mu, then ν1=νac\nu_1 = \nu_{ac} and ν2=νs\nu_2 = \nu_s.

The Lebesgue Decomposition separates any measure into components that are "compatible" with μ\mu (the absolutely continuous part) and "incompatible" with μ\mu (the singular part). This is fundamental for understanding the structure of measures.

ExampleDiscrete and Continuous Parts

On R\mathbb{R} with Lebesgue measure λ\lambda, consider: ν=12λ+12δ0\nu = \frac{1}{2}\lambda + \frac{1}{2}\delta_0

where δ0\delta_0 is the Dirac measure at 00. Then:

  • νac=12λ\nu_{ac} = \frac{1}{2}\lambda (absolutely continuous with respect to λ\lambda)
  • νs=12δ0\nu_s = \frac{1}{2}\delta_0 (singular with respect to λ\lambda)

The Radon-Nikodym derivative is: dνacdλ=12\frac{d\nu_{ac}}{d\lambda} = \frac{1}{2}

This models a probability distribution with both continuous and discrete components.

Remark

Important consequences and applications:

  1. Every measure decomposes: Any measure ν\nu on R\mathbb{R} can be written as ν=νac+νsc+νd\nu = \nu_{ac} + \nu_{sc} + \nu_d where:

    • νac\nu_{ac} is absolutely continuous (has a density)
    • νsc\nu_{sc} is singular continuous (like the Cantor-Lebesgue function)
    • νd\nu_d is discrete (sum of point masses)
  2. Probability distributions: In probability, every distribution function FF decomposes into absolutely continuous (with PDF), singular continuous, and jump components.

  3. Spectral theory: The spectral measure of a self-adjoint operator decomposes into absolutely continuous, singular continuous, and pure point spectra.

  4. Harmonic analysis: The Lebesgue decomposition helps classify measures in terms of their Fourier transform properties.

  5. Optimal transport: The decomposition is used to understand the structure of optimal transport plans.

The Lebesgue Decomposition Theorem, together with Radon-Nikodym, provides a complete understanding of how two measures relate to each other, forming a cornerstone of modern measure theory.