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Equipartition identity with explicit integrated boundary terms

Statement

Let (Y,G,ν) be a sigma-finite measure space, β>0, and H:R×Y→R a product-measurable function whose map z↦H(z,y) is C1 for ν-almost every y. Set Z:=∫R×Ye−βH(z,y) d(z,y)∈(0,∞), where d(z,y) is Lebesgue measure on R times ν. Assume ∫R×Y∣z∂zH(z,y)∣e−βH(z,y) d(z,y)<∞. For R>0 let BR:=∫Y(Re−βH(R,y)+Re−βH(−R,y)) dν(y), and assume BR→0 as R→∞. Define ⟨F⟩β:=Z−1∫F(z,y)e−βH(z,y) d(z,y) whenever the integral is absolutely convergent. Then ⟨z∂zH⟩β=β−1. For finite endpoints a<b, assume the endpoint integral below is finite and put Z[a,b]:=∫[a,b]×Ye−βH d(z,y). If 0<Z[a,b]<∞, define ⟨F⟩[a,b]:=Z[a,b]−1∫[a,b]×YFe−βH d(z,y). Then the exact boundary identity is ⟨z∂zH⟩[a,b]=β−1(1−Z[a,b]−1∫Y(be−βH(b,y)−ae−βH(a,y)) dν(y)),

Facts & Assumptions

Given: The product measure space, β, H, the finite positive normalization Z, the integrable moment, and the vanishing integrated boundary term BR.

[A1]

The measure factors are sigma-finite, H is measurable and sectionwise C1, and Z and ∫∣zHz∣e−βH are finite with Z>0.

[A2]

The two integrated endpoint contributions tend to zero, equivalently BR→0.

[A3]

For the finite-interval clause, 0<Z[a,b]<∞ and the stated integrated endpoint expression is finite.

[F1]

Tonelli's theorem permits section integration for nonnegative product-measurable functions on sigma-finite factors (Tonelli's theorem for nonnegative measurable functions on a sigma-finite product).

[F2]

Dominated convergence passes limits through an integral under one common integrable majorant (Dominated convergence).

Proof

Given: [A1]–[A3] and the Tonelli and dominated-convergence interfaces [F1]–[F2].

1.1A1algebra

For almost every y, differentiate the product in the z coordinate: ∂z(ze−βH(z,y))=e−βH(z,y)−βz∂zH(z,y)e−βH(z,y). The absolute value of the right side is bounded by (1+β∣z∂zH∣)e−βH, which is integrable by [A1].

2.1A1F1step 1.1

Integrate this identity on [−R,R]×Y. Absolute integrability and [F1] justify integrating first in z and then in y, so ∫[−R,R]×Ye−βH d(z,y)−β∫[−R,R]×Yz∂zHe−βH d(z,y)=∫Y(Re−βH(R,y)+Re−βH(−R,y)) dν(y)=BR.

3.1A1A2F2step 2.1

The integrand in the first term is nonnegative and integrable, while the second integrand is absolutely integrable by [A1]. Their restrictions to [−R,R]×Y converge pointwise almost everywhere to the full integrands and are dominated by those integrable functions. Applying [F2] to both terms and using [A2] gives Z−β∫z∂zHe−βH d(z,y)=0. Divide by βZ>0 to obtain the stated identity.

4.1A1A3F1step 1.1algebra∎

For finite a<b, integrate the same derivative over [a,b]×Y. The boundary evaluation is ∫Y(be−βH(b,y)−ae−βH(a,y)) dν(y)=Z[a,b]−β∫[a,b]×Yz∂zHe−βH d(z,y). Dividing by βZ[a,b] and rearranging yields the displayed finite-endpoint formula.

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