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Dominated exponential normalization and covariance

Statement

Let (Ω,F,m) be a sigma-finite measure space, let w≥0 be measurable with m({w>0})>0, let r≥1 and let X=(X1,…,Xr):Ω→Rr be measurable and finite, and let Θ⊆Rr be open. For each compact K⊂Θ, assume an integrable GK satisfies w(x)eθ⋅X(x)(1+∑a∣Xa(x)∣2)≤GK(x)(θ∈K). Then Z(θ)=∫weθ⋅X dm is finite, strictly positive and C2, and the probability density ρθ=Z(θ)−1weθ⋅X defines dPθ=ρθ dm as in The measure with density f relative to μ. For any integrable real A, write ⟨A⟩θ:=∫A dPθ; for square-integrable real A,B, define Cov⁡θ(A,B):=∫(A−⟨A⟩θ)(B−⟨B⟩θ) dPθ. These extend the phase-space conventions of Statistical states, densities, observables and expectations to the present measure space. Then ∂alog⁡Z=⟨Xa⟩θ,∂a∂blog⁡Z=Cov⁡θ(Xa,Xb). In particular, the Hessian of log⁡Z is positive semidefinite.

Facts & Assumptions

Given: The measurable model above and one common integrable envelope on each compact parameter neighborhood.

[A1]

For every compact K⊂Θ, the stated GK is integrable and dominates the zeroth, first and second exponential moments.

[F1]

Dominated convergence passes pointwise limits through an integral when the functions have a common integrable majorant (Dominated convergence).

[F4]

The measure with density is defined on an arbitrary measure space (The measure with density f relative to μ). Integration against it equals integration of the density-weighted nonnegative function (Integrating against a density agrees with integrating the product); applying this to positive and negative parts gives the same identity for integrable real functions. Expectations and covariances here have the explicit integral definitions in the Statement, agreeing with Statistical states, densities, observables and expectations when the reference is a phase-reference space.

Proof

Given: [A1] and the integration, exponential and state interfaces [F1]–[F4].

1.1A1F3algebra

For each fixed θ∈Θ, choose a compact neighborhood K of θ. The bound in [A1] implies ∫weθ⋅Xdm<∞. On {w>0} the integrand is strictly positive by [F3]; since this set is the countable union of the sets {weθ⋅X≥1/k}, at least one has positive measure. Hence Z(θ)>0 as well as finite.

2.1A1F1F2step 1.1algebra

For coordinate a, choose a compact neighborhood K of θ containing every θ+sea with ∣s∣≤ϵ. The mean-value theorem and chain rule [F2] bound the difference quotient by w∣Xa∣sup⁡∣s∣≤ϵe(θ+sea)⋅X. Since ∣Xa∣≤1+∑c∣Xc∣2, [A1] bounds this entire supremum pointwise by the single integrable GK. Thus [F1] gives ∂aZ=∫wXaeθ⋅Xdm. Applying the same argument to the first derivative, with ∣XaXb∣≤(∣Xa∣2+∣Xb∣2)/2, gives ∂b∂aZ=∫wXaXbeθ⋅Xdm. The same local envelopes and [F1] give continuity of these derivatives, hence Z∈C2.

3.1F3F4step 2.1algebra∎

By [F3], dividing the first-derivative formula by Z>0 gives ∂alog⁡Z=⟨Xa⟩θ. Differentiating once more yields ∂b∂alog⁡Z=∫XaXbweθ⋅XdmZ−∫Xaweθ⋅Xdm∫Xbweθ⋅XdmZ2=⟨XaXb⟩−⟨Xa⟩⟨Xb⟩. The envelope makes ∫Xa2 dPθ finite; ∣Xa∣≤1+Xa2 and 2∣XaXb∣≤Xa2+Xb2 give finite means and mixed moments. Expanding the centered product in the Statement's covariance definition, and using Pθ(Ω)=1, identifies the displayed difference with that covariance. For v∈Rr its quadratic form is ⟨(v⋅(X−⟨X⟩))2⟩≥0, proving positive semidefiniteness.

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