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Specific Relative Entropy Density
Statement
Assume AC and let , with this class defined in Local-Tame Topology, be stationary for the translations of Poisson Configuration Reference. For a bounded Borel set , write and for the restrictions of and the unit-intensity Poisson reference to configurations in . For , put and Then the specific relative entropy density exists in and satisfies If , every bounded Borel restriction has finite relative entropy. This is an information functional relative to the specified unit-intensity Poisson law; changing the reference changes its value.
Facts & Assumptions
Given: AC, dimension , a stationary finite-intensity configuration law , and the unit-intensity reference .
The Axiom of Choice is inherited from the standard-Borel Poisson reference and its countable product construction (The Axiom of Choice, Poisson Configuration Reference).
For independent Poisson reference restrictions on disjoint bounded sets, the finite-region relative entropy is nonnegative, obeys the conditional chain rule, and does not increase under restriction (Poisson Reference Counts and Translation Invariance, Relative Entropy of Probability Measures, Relative Entropy Variational, Chain, and Conditioning Rules).
For the stated dimension , the domain consists of translation-invariant laws with finite unit-cell count, and stationarity of and gives for every bounded Borel and translation (Local-Tame Topology, Poisson Configuration Reference, Poisson Reference Counts and Translation Invariance).
If a cube restriction has finite relative entropy, then every bounded subregion has no larger relative entropy (Relative Entropy Variational, Chain, and Conditioning Rules, claim 2).
Proof
Given: AC, , and as in the Statement.
If are disjoint bounded Borel sets, [F1] decomposes into plus the mean conditional relative entropy of given . That conditional increment is at least by the conditioning monotonicity in [F1], comparing observation by with no observation. Thus relative entropy is superadditive over disjoint regions; if the left side is infinite the inequality is immediate, and otherwise all terms in the chain rule are finite.
Fix an integer and let . Tile by disjoint translates of , leaving the Borel remainder . Iterating step 1.1 and using nonnegativity on the remainder gives because stationarity gives the same entropy for each translated -cube. If , this forces for every .
Put . If , step 2.1 makes the liminf of exceed every finite bound, so the integer-cube limit is . If , step 2.1 gives for every , since . Taking the supremum gives liminf at least , while the definition of gives for every integer . Hence the integer-cube limit exists and equals .
For real , let . The inclusions and [F3] give . Since and , step 3.1 squeezes to the same extended limit ; if some integer-cube entropy is infinite, monotonicity gives the same conclusion directly.
If and is bounded, choose an integer cube containing . Stationarity [F2] and restriction monotonicity [F3] give Thus every bounded restriction has finite relative entropy.