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Periodic preparation and local-tame transfer from entropy bounds

Statement

Assume AC, the ultrafilter extension principle, DC, and HB as in Compactness of Finite-Specific-Entropy Levels in the Local-Tame Topology. Let L→∞ and let CL be probability laws on finite configurations in ΛL=[0,L)d, invariant under every translation modulo LZd. Write QL for unit-intensity Poisson measure and suppose cL=L−dD(CL∥QL),sup⁡LcL<∞. Let C~L be the law of the periodic continuation. Then C~L=ECLRL,ω; these laws are stationary and are relatively sequentially compact in τL as L→∞. Their local counts are uniformly integrable. Along any convergent subsequence with limit P, I(P)≤lim inf⁡LcL. If the empirical fields RL,ω converge in probability in τL to a fixed P∗, then C~L→P∗ in τL, including expectations of every measurable local f with ∣f∣≤b(1+NA) for bounded A. This concerns periodic continuation, not the zero extension of a configuration outside its fundamental cube.

Facts & Assumptions

Given: The stated choice hypotheses, torus-invariant laws, and bounded entropy densities.

[F1]

Periodized empirical field of a finite configuration and Stationarity and intensity of a periodized empirical field: the empirical field averages translations of the periodic continuation; its barycenter is stationary with intensity ECLN/Ld when this expectation is finite.

[F2]

Relative Entropy Variational, Chain, and Conditioning Rules: relative entropy decreases under restriction, is superadditive over disjoint regions against a product reference, and satisfies the bounded-test variational inequality.

[F3]

Poisson Reference Counts and Translation Invariance: Poisson counts have all positive exponential moments.

[F4]

Dunford--Pettis for real L1 on a finite measure space and Eberlein–Šmulian theorem: under the named choice hypotheses, uniformly integrable real L1 densities on a probability space have weakly compact closures and weakly convergent subsequences. Weak topology on a normed space and Holder's inequality for integrals, including the endpoint cases make bounded measurable tests weakly continuous. The cell spaces in Poisson Configuration Reference are standard Borel; Assuming the Axiom of Choice, Kolmogorov extension for arbitrary families of standard Borel coordinate spaces extends their consistent finite-dimensional laws under AC. The local extraction required here is proved in steps 3.2 and 4.1, rather than attributed to compactness of specific-entropy levels.

[F5]

Specific Relative Entropy Density: for a stationary law, I(P)=sup⁡a∈N, a≥1a−dD(P[0,a)d∥Q[0,a)d).

[F6]

Monotone convergence for the integral and Dominated convergence: bounded count truncations may increase to counts, and Poisson exponential domination justifies the tail limits below.

Proof

Given: The hypotheses and suppliers in Facts & Assumptions.

1.1givenF1F2F3F6algebra

For bounded local f, torus invariance gives ECLf(Txω(L))=ECLf(ω(L)) for every x. Integrating over ΛL proves C~L(f)=ECLRL,ω(f). In particular the continued law is stationary. The entropy inequality with bounded truncations of aNΛL and [F3] gives finite ECLN, so the intensity assertion of [F1] applies.

2.1F2step 1.1algebra

Fix an integer a≥1 and take L>a. The fundamental cube contains mL=⌊L/a⌋d disjoint translates of W=[0,a)d. Their Poisson restrictions are independent and their CL marginals are identical by torus invariance. Superadditivity gives D((C~L)W∥QW)≤D(CL∥QL)/mL=cLLd/mL. For fixed a, Ld/mL→ad. Translation invariance gives the same bound for every translate of W, hence a uniform entropy bound on every bounded region.

3.1F2F3F6step 2.1algebra

On a bounded A⊂W, apply the entropy inequality to tmin⁡(NA1{NA>K},M) and let M→∞. If CW is the uniform bound from step 2.1, then tEC~L[NA1{NA>K}]≤CW+log⁡EQWetNA1{NA>K}. For fixed t>0, the logarithm tends to zero as K→∞ by [F3] and [F6]. First take t large and then K large. This proves uniform count-tail integrability.

3.2A1F2F4step 2.1algebra

Consider any sequence of periods tending to infinity and enumerate the integer cubes W=a+[0,m)d. For each fixed W, step 2.1 gives a finite entropy bound CW on an eventual tail; it does not assert a bound for all periods on arbitrarily large cubes. For a probability density h=dPW/dQW with entropy at most CW, the inequalities −ulog⁡u≤1/e for 0≤u≤1 and hlog⁡h≥hlog⁡K on {h>K} give ∫h>Kh dQW≤(CW+1/e)/log⁡K. These densities have norm one and are uniformly integrable. By [F4], discard the finite exceptional prefix for the first cube and extract a weakly convergent subsequence, then do so for the second cube and continue; diagonal extraction, using AC, gives weak convergence on every cube. Each limiting density is nonnegative with integral one, by tests against indicators and 1. The entropy variational formula [F2] is a supremum of weakly continuous affine functions, so it gives entropy at most CW for each limit.

4.1A1F2F4F5step 2.1step 3.1step 3.2construct

Consistency of restrictions and stationarity pass to these limits by testing bounded measurable local functions: every equality involves only finitely many cube coordinates. A finite set of unit cells lies in an integer cube; its induced marginal is independent of the containing cube by consistency through a larger cube. The standard-Borel extension [F4] gives a law on the countable cell product, hence on simple locally finite configurations. It is stationary. The bound of step 3.1 holds for its cube marginals as well, so its counts are integrable and their tails are controlled. Truncating f on {NA≤K} therefore upgrades bounded-local convergence of the extracted sequence to convergence for every tame f, by step 3.1. This proves relative sequential compactness as the periods tend to infinity. Along any such convergent sequence, the same variational formula gives D(PW∥QW)≤lim inf⁡D((C~L)W∥QW). Taking a further subsequence realizing lim inf⁡cL, step 2.1 gives a−dD(P[0,a)d∥Q[0,a)d)≤lim inf⁡cL for every integer a≥1; [F5] yields I(P)≤lim inf⁡cL.

5.1step 1.1step 3.1step 4.1algebra∎

If the empirical fields converge in probability to P∗, then for bounded local f the bounded random variables RL,ω(f) converge in probability to P∗(f), hence their expectations converge. By step 1.1 this is convergence of C~L(f). For tame f, truncate on {NA≤K}; step 3.1 makes the truncation error uniformly small, and the same is true for the limit law. Taking L→∞ and then K→∞ proves convergence for every stated tame observable.

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