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The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
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- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Finite Gibbs response and covariance identities
Statement
Let be finite nonempty, let , fix , and set and for . For the normalized finite Gibbs law , where . For fixed , the corresponding inverse-temperature identities are These are finite-state identities; they do not justify differentiating an infinite-volume limit.
Facts & Assumptions
Given: A finite nonempty state set, real-valued observables and energies, and a positive finite parameter .
For finite energies and , the finite Gibbs weights normalize to a strictly positive probability law (Finite Gibbs relative entropy and free-energy minimum).
The real exponential is differentiable with derivative (The exponential function is smooth and ).
The natural logarithm is differentiable on with derivative (The natural logarithm has derivative 1/x and equals the integral from 1 to x of 1/t).
Finite sums, products, quotients with nonzero denominator, and compositions of differentiable real functions obey the sum, product, quotient, and chain rules (Sums, scalar multiples, products and quotients: , , , and when , The chain rule, in one line from Carathéodory: if is differentiable at and is differentiable at , then is differentiable at with ).
Proof
Since is finite, repeated use of the sum rule and chain rule [F1, F3] differentiates each summand and gives . Positivity of follows from [A1]; the logarithm chain rule and [F2, F3] give .
Differentiate the finite-sum numerator and denominator by [F1, F3], then apply the quotient rule from [F3]. This gives . Multiplying by the factor in step 1.1 gives the stated second derivative, which is nonnegative because it equals .
For the inverse-temperature family, finite-sum differentiation using [F1, F3] gives and . Applying the logarithm chain rule and quotient rule from [F2, F3] yields the stated mean and variance identities.
Depends on
Finite Gibbs relative entropy and free-energy minimum
The exponential function is smooth and
The natural logarithm has derivative 1/x and equals the integral from 1 to x of 1/t
Sums, scalar multiples, products and quotients: , , , and when
The chain rule, in one line from Carathéodory: if is differentiable at and is differentiable at , then is differentiable at with