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GJ §18.4–18.5: general interacting cluster-expansion convergence (Kotecký–Preiss / tree-graph) #3954

Description

@phasetr

Purpose

Establish the general interacting Mayer/cluster expansion identity and its
convergence — the capstone of GJ §18.4–18.5 (the Mayer–Montroll exponential
formula Ξ = exp(∑ cluster terms) / log Ξ = ∑_n mayerExpansionTerm, valid for
arbitrary activity t in a convergence regime), for an interacting polymer gas
(not just the non-interacting / vertex-disjoint case already done).

Background

The non-interacting case is complete (MayerCore/Independent*.lean,
PRs #3945#3948, #3951): there the Mayer expansion converges to the polymer free
energy by the diagonal collapse + single-polymer log(1+t^|P|) series. The
finite-order coefficients are also done: the n = 3 Ursell classification
(#3949, #3950, #3952) and the closed form of the third (first interacting) Mayer
term (#3953), plus the n = 2 term (Step 593/614).

The general interacting case needs a genuine convergence criterion. The naive
Ursell bound |ϕ^T(ω)| ≤ 2^|E(G(ω))|/n! (Step 603) does not give absolute
convergence of ∑_n ∑_ω |ϕ^T(ω)|·|z(ω)|. The standard routes are:

  • Kotecký–Preiss criterion: a function a(P) > 0 with
    ∑_{Q ≁ P} |z(Q)| e^{a(Q)} ≤ a(P) for every polymer P, giving
    ∑_{Γ ∋ P} |ϕ^T(Γ)| ∏ |z| ≤ a(P) and hence absolute convergence + analyticity.
  • Penrose / tree-graph inequality: |∑_{connected S} (-1)^|S|| ≤ #{spanning trees}
    bounding the Ursell coefficient by a sum over tree subgraphs.

Tracking (PR checklist)

References

  • Glimm–Jaffe, Quantum Physics, 2nd ed., §18.4 ("Convergence: The Main Ideas", p. 332) – §18.5 (p. 335).
  • Friedli–Velenik, Statistical Mechanics of Lattice Systems, §5.7 (cluster expansion, KP).
  • Kotecký–Preiss, Cluster expansion for abstract polymer models, CMP 103 (1986).
  • Penrose tree-graph inequality (Brydges' lectures).

Part of the broader §18 cluster-expansion programme (Issue #1499).

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