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).
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 forarbitrary activity
tin 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. Thefinite-order coefficients are also done: the
n = 3Ursell classification(#3949, #3950, #3952) and the closed form of the third (first interacting) Mayer
term (#3953), plus the
n = 2term (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 absoluteconvergence of
∑_n ∑_ω |ϕ^T(ω)|·|z(ω)|. The standard routes are:a(P) > 0with∑_{Q ≁ P} |z(Q)| e^{a(Q)} ≤ a(P)for every polymerP, giving∑_{Γ ∋ P} |ϕ^T(Γ)| ∏ |z| ≤ a(P)and hence absolute convergence + analyticity.|∑_{connected S} (-1)^|S|| ≤ #{spanning trees}bounding the Ursell coefficient by a sum over tree subgraphs.
Tracking (PR checklist)
alternatingConnectedSubgraphSum(Ursell numerator) — M1 (feat(gj-18.4): Penrose Boolean-interval cancellation + spanning-tree API — #3954 #3987-feat(gj-18.4): Penrose tree-graph inequality |altSum| ≤ numSpanningTrees — #3954 #3992) + Ursell tree bound (feat(gj-18.4): Ursell tree bound from the Penrose inequality — #3954 #3993)e·∑_P|t|^{|P|} < 1(feat(gj-18.4): absolute convergence of the Mayer expansion — #3954 #3996), via K_n count bound (feat(gj-18.4): K_n spanning-tree count bound n^(n-1) via parent injection — #3954 #3994) + summable majorant radius 1/e (feat(gj-18.4): summable Mayer majorant — radius 1/e via ratio test — #3954 #3995)∑_n mayerExpansionTermunder KP —summable_mayerExpansionTerm_of_exp_one_mul_activity_lt_one(feat(gj-18.4): absolute convergence of the Mayer expansion — #3954 #3996, general interacting)log Ξ = ∑_n mayerExpansionTerm(generalt, KP regime) —mayer_identity_general_t(MayerMontroll.lean, Issue Mayer expansion general-t identity for log Ξ (GJ §18.4 capstone) #1499 Phase C, PR feat(gj-18.4): Mayer–Montroll cluster identity log Ξ = ∑ₙ mayerExpansionTerm (general t) — #1499 #3998) + per-site KP formpolymerFreeEnergy_eq_tsum_mayerExpansionTerm_of_persite_kp(MayerIdentityPersiteKP.lean, PR feat(gj-18.6): volume-uniform per-site KP Mayer-Montroll identity — #4149 #4152)tanh(βJ)—summable_mayerExpansionTerm_tanh(feat(gj-18.4): high-temperature convergence of the Ising cluster expansion — #3954 #3997)polymerFreeEnergy/freeEnergyReferences
Part of the broader §18 cluster-expansion programme (Issue #1499).