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Root-L2 Hellinger distance between density laws

Definition

Let (X,A,μ) be a measure space and let p,q:X→[0,∞) be measurable densities with ∫p dμ=∫q dμ=1. They define probability laws P(B)=∫Bp dμ and Q(B)=∫Bq dμ (Probability measures and probability spaces). Their root-L2 Hellinger distance, with the root-L2 normalization, is h(P,Q):=(∫X(p−q)2 dμ)1/2.

The dominating measure μ is fixed throughout a use of this definition. Changing either density on a μ-null set does not change the value, since the integrand changes only on a null set. This definition does not assert that separate choices of density versions are jointly measurable in an additional parameter.

Remarks

The integrand is measurable: square root is Borel on [0,∞), and subtraction and squaring preserve measurability (Composition with a Borel measurable outer map preserves measurability, Arithmetic and lattice operations preserve measurability whenever they are defined). For a,b≥0, (a−b)2=a+b−2ab≤a+b. Thus 0≤(p−q)2≤p+q pointwise; monotonicity and additivity of the nonnegative integral (Monotonicity and nonnegative homogeneity of the nonnegative integral, Additivity of the nonnegative Lebesgue integral) give h(P,Q)2≤∫(p+q) dμ=2, so the defining integral is finite. The set functions B↦∫Bp dμ and B↦∫Bq dμ are measures by The measure with density f relative to μ, and their total masses are one, so they are probability laws by Probability measures and probability spaces. Changing either density on a μ-null set changes the integrand only on a null set, whose nonnegative integral vanishes (A nonnegative integral over a null set vanishes), confirming the stated version invariance.

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