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Full uniform phase shell has vanishing specific canonical KL

Statement

Assume AC and the hypotheses and notation of Total-energy concentration and controlled canonical windows. Let Rn=RLn,Nn be the finite phase reference of Interacting marked phase-space and reference measures, let An be the constructed band, and set Mnph(E)=Rn(E∩An)/Rn(An). Let Cnph be the full fixed-Nn canonical probability. Then Dn=D(Mnph∥Cnph) satisfies Dn/Vn→0. This is a mathematical statement about a normalized measure restriction; it does not assert Dn→0 or global total-variation convergence.

Facts & Assumptions

Given: AC, the finite-reference phase measure, the canonical law, stability, and the window hypotheses.

[A1]

AC is used by the conditional entropy chain rule (The Axiom of Choice).

[F1]

Total-energy concentration and controlled canonical windows: Cnph(An)→1, δn→0, and An is a finite positive-reference-measure energy band ∣H/Vn−eb∣≤δn at fixed Nn.

[F2]

Interacting marked phase-space and reference measures: relative to phase reference Rn, Cnph has density e−bH/Zn; by the definition in the Statement, Mnph=Rn(⋅∩An)/Rn(An).

[F3]

Relative Entropy of Probability Measures and Conditional entropy chain and disjoint-block bounds: relative entropy is nonnegative and the exact directional convention is D(P∥Q).

Proof

Given: The hypotheses and supplier definitions above.

1.1F1F2algebra

On A_n, the density of M_n^ph relative to C_n^ph is Z_n e^{bH}/R_n(A_n). Therefore Dn=−log⁡Rn(An)+log⁡Zn+bEMnphH. The lower band edge gives Rn(An)=ZnECnph[1AnebH]≥ZnCnph(An)ebVn(eb−δn).

2.1A1F1F3step 1.1algebra∎

The upper band edge gives EMnphH≤Vn(eb+δn). Substituting the step 1.1 lower bound for Rn(An) yields Dn≤−log⁡Cnph(An)+2bVnδn. Relative entropy is nonnegative by [F3]; since Cnph(An)→1 and δn→0 by [F1], this proves 0≤Dn/Vn→0.

Depends on

Dependency tree · 2 levels

Sources