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LemmaStatement: AI-adaptedProof: AI-adaptedPipeline-generatedverified 2026-10-22 (gpt-6.1-sol)
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Finite Gibbs response of an observable is β times its covariance with the field-coupled observable

Statement

Let E be a finite nonempty set, let H0,M,F:E→R, fix β>0, and for t∈R define Ht(x):=H0(x)−tM(x), Z(t):=∑x∈Ee−βHt(x), and γt(x):=Z(t)−1e−βHt(x). For functions F,M:E→R, define Cov⁡γt(F,M):=∑xγt(x)F(x)M(x)−(∑xγt(x)F(x))(∑xγt(x)M(x)). Then t↦∑xγt(x)F(x) is differentiable on R and

ddt∑x∈Eγt(x)F(x)=βCov⁡γt(F,M).

Facts & Assumptions

Given: A finite nonempty set E, real-valued functions H0,M,F:E→R, and β>0.

[F1]

For every finite nonempty state set and finite real energy, the Gibbs partition sum is finite and strictly positive, and its normalized weights form a probability vector (Finite Gibbs relative entropy and free-energy minimum).

[F2]

The real exponential is differentiable with derivative exp⁡ (The exponential function is smooth and (exp⁡)′=exp⁡).

Proof

1.1givenF1algebra

For every t∈R, each e−βHt(x) is positive and finite, and E is finite nonempty, so 0<Z(t)<∞ by [F1]. Thus γt is a probability vector, and both Z(t) and NF(t):=∑xF(x)e−βHt(x) are finite sums with nonzero denominator Z(t).

2.1F2F3F4step 1.1

Since Ht(x)=H0(x)−tM(x), [F2] and [F4] give ddte−βHt(x)=βM(x)e−βHt(x). Differentiating the finite sums term by term with [F3] therefore gives Z′(t)=β∑xM(x)e−βHt(x) and NF′(t)=β∑xF(x)M(x)e−βHt(x).

3.1F3step 1.1step 2.1∎

The denominator Z(t) is nonzero by step 1.1. The quotient rule [F3] applied to NF(t)/Z(t)=∑xγt(x)F(x) yields β{γt(FM)−γt(F)γt(M)} after dividing numerator and denominator by Z(t); by the definition of covariance in the Statement this is βCov⁡γt(F,M).

Depends on

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