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Finite-site microcanonical and canonical block equivalence

Statement

Let A={1,…,q}, q≥1, have real energies ej, and fix finite β∈R. Set Z1=∑je−βej, pj=e−βej/Z1>0, and E=∑jpjej. For each N≥1, let δN≥q∑j=1q∣ej∣ and δN/N→0. Define the shell ΓN={i∈AN:∣∑r=1Neir−NE∣≤δN} and the uniform law on that shell. For probability laws μ,ν on the finite set Ak, total variation distance means 12∑x∈Ak∣μ(x)−ν(x)∣. Then ΓN is nonempty for every N; for each fixed k≥1, the first k-site marginal (for N≥k) converges in that distance to p⊗k; and 1Nlog⁡∣ΓN∣⟶H(p):=−∑j=1qpjlog⁡pj. The conclusion is for this finite alphabet, additive energy, exact shell width and uniform shell law. It does not assert finite-size equality or equivalence for interacting or continuous models.

Facts & Assumptions

Given: The finite-site canonical law and uniform shell convention.

[A1]

A is finite, q≥1, ej∈R, β∈R, and δN≥q∑j∣ej∣ with δN/N→0.

[F1]

Finite-site canonical law and microcanonical shell: configurations have additive energies, the canonical probabilities are pj=e−βej/Z1, and the shell law is uniform when the shell is nonempty.

[F2]

Finite sums and finite products, by recursion and Order, continuity, range, and the product, quotient, and reciprocal laws for the natural logarithm: the finite sums and logarithms obey the usual finite distributive and product identities.

[F3]

The real exponential function and the number e by a power series and The natural logarithm as the inverse of the exponential function: exponential weights are positive and logarithm is the inverse of the positive real exponential.

[F4]

The natural logarithm has derivative 1/x and equals the integral from 1 to x of 1/t: log⁡ is continuous on (0,∞), has derivative 1/x, and log⁡x=∫1xdt/t.

[F5]

Heine-Borel in Rn: with the Euclidean metric a subset of Rn is compact if and only if it is closed and bounded, and the proof by bisection uses no choice principle; the same holds on the real line: the finite-dimensional probability simplex is closed and bounded, hence compact; closed bounded subsets of finite-dimensional Euclidean space are compact.

[F6]

A continuous real-valued function on a nonempty compact metric space is bounded and attains a greatest and a least value: a continuous real-valued function on a nonempty compact metric space attains its minimum and maximum.

Proof

Given: [A1] and the conventions in [F1].

1.1A1F2F3F4algebra

For a type tj=nj/N, the number of configurations of that type is M(n)=N!/∏jnj!. The increasing function log⁡x gives ∫1mlog⁡x dx≤log⁡(m!)≤∫1m+1log⁡x dx(m≥1). Evaluating the antiderivative xlog⁡x−x and using log⁡(1+1/m)≤1/m shows log⁡(m!)=mlog⁡m−m+O(log⁡(m+1)+1) with an absolute constant; the case m=0 uses 0!=1 and 0log⁡0=0. Subtracting the q denominator estimates from the numerator estimate gives a constant Cq such that NH(t)−Cqlog⁡(N+1)−Cq≤log⁡M(n)≤NH(t)+Cqlog⁡(N+1)+Cq, where H(t)=−∑jtjlog⁡tj. The sharper upper bound M(n)≤eNH(t) follows by expanding 1=(∑jtj)N and retaining the nonnegative terms with counts n. For later limits, [F4] gives 0≤log⁡x=∫1xdt/t≤2x for x≥1, hence log⁡(N+1)/N≤2N+1/N→0.

1.2A1F1F2F3F4

For any probability vector t, define D(t∥p)=∑j:tj>0tjlog⁡(tj/pj). From [F4], log⁡u≥1−1/u for u>0, with equality only at u=1: apply log⁡z≤z−1 to z=1/u and negate. Therefore D(t∥p)≥∑j:tj>0(tj−pj)=1−∑j:tj>0pj≥0. Since every pj>0, equality forces every index into the support and tj/pj=1 for each j, so t=p. Also log⁡pj=−βej−log⁡Z1, hence D(t∥p)=−H(t)+β∑jtjej+log⁡Z1. In particular, among types of exact mean energy E, entropy is at most H(p), with equality only at p.

2.1A1F1F4step 1.1

Round down Npj for j<q and put the remainder in nq. Then ∣nj/N−pj∣≤1/N for j<q and ∣nq/N−pq∣≤(q−1)/N. Thus ∣∑jnjej−NE∣≤∑j<q∣ej∣+(q−1)∣eq∣≤q∑j∣ej∣≤δN. This type belongs to ΓN, proving nonemptiness. Its frequencies tend to p. For 0<x≤1, [F4] gives 0≤−xlog⁡x=xlog⁡(1/x)≤2x, by integrating 1/t≤1/t on [1,1/x]; hence −xlog⁡x extends continuously by 0 at x=0 and H(t)→H(p). By the lower bound in 1.1, the shell contains at least exp⁡(NH(p)−o(N)) configurations.

3.1A1F1F4F5F6step 1.1step 2.1step 1.2

Fix ϵ>0 and let Δq={t∈[0,1]q:∑jtj=1} and C={t∈Δq:∣t−p∣≥ϵ}. The simplex is closed and bounded, and C is closed in it, so both are compact by [F5]. If C=∅, the claim is vacuous. Otherwise let F={t∈C:∑jtjej=E}, a closed subset of C. If F=∅, the continuous function t↦∣∑jtjej−E∣ has a positive minimum on C by [F6], so choose τ smaller than this minimum and any η>0. If F≠∅, [F6] gives a maximum hF of H on F; step 1.2 gives hF<H(p). Put η=(H(p)−hF)/2 and let U={t∈C:H(t)<H(p)−η}, a relative open neighborhood of F. The compact set C∖U, if nonempty, has a positive minimum m of ∣∑jtjej−E∣ by [F6]; choose 0<τ<m. If C∖U=∅, choose any τ>0. In either case, every t∈C with ∣∑jtjej−E∣≤τ satisfies H(t)≤H(p)−η. For large N, δN/N≤τ; therefore every shell type outside the ϵ-ball has entropy at most H(p)−η. There are at most (N+1)q types, and 1.1 bounds the number of configurations of each by exp⁡[NH(t)]. By the log-growth estimate in 1.1, this type-count factor is subexponential, so division by the shell lower bound in step 2.1 shows that the shell probability outside the ball tends to zero exponentially. Thus the random type converges in probability to p.

4.1A1F1F5step 3.1algebra

Conditional on a type t, a uniform configuration is a uniformly ordered list of its N labeled positions. Couple the first k draws without replacement with k independent uniform position draws: if the independent positions are distinct, keep them; if not, replace them by an independently chosen uniform ordered distinct k-tuple. The resulting tuple is uniform among distinct positions and agrees with the original draws except on the collision event. A union bound over the (k2) pairs gives collision probability at most k(k−1)/(2N). Hence the type-conditional label marginal differs in total variation from t⊗k by at most this quantity. Since t→p in probability, for each fixed tuple (i1,…,ik)∈Ak the random variable XN=∣∏r=1ktir−∏r=1kpir∣ tends to zero in probability and is bounded by 1. For every ϵ>0, EXN≤ϵ+P(XN>ϵ), so EXN→0; summing over the finite set Ak proves the marginal converges to p⊗k in total variation.

5.1A1F1F4F5step 1.1step 1.2step 2.1algebra∎

The rounded shell type and lower bound in step 2.1 give lim inf⁡NN−1log⁡∣ΓN∣≥H(p). For any shell type t, step 1.2 gives the exact identity H(t)=H(p)+β(∑jtjej−E)−D(t∥p)≤H(p)+∣β∣δN/N. There are at most (N+1)q types, and step 1.1 bounds each multiplicity by eNH(t). Therefore ∣ΓN∣≤(N+1)qexp⁡ ⁣(NH(p)+∣β∣δN). By the log-growth estimate in 1.1, qlog⁡(N+1)/N→0. Since also δN/N→0, the limsup is at most H(p). Together with the lower bound this proves the entropy-density limit, including β=0, without invoking a nonexistent compactness step.

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