Alphabeta Math
DefinitionDefinition: Literature-sourcedProof: Not applicablePipeline-generatedprecheck passverified 2026-10-22 (gpt-6.1-sol)
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Free, wired, and subsequential infinite-volume FK states on the square lattice

Definition

Let E∞ be the nearest-neighbor edge set of Z2, and let Λn=[−n,n]2∩Z2. Let En contain the edges with both endpoints in Λn, and let ∂Λn be the vertices of Λn adjacent to a vertex outside it. Fix q≥1 and p∈(0,1). For each boundary partition ξn on ∂Λn, let ϕn,p,qξn be the finite FK law on (Λn,En) with mass proportional to p∣A∣(1−p)∣En∖A∣qkξn(A) for A⊆En, where kξn(A) counts components after wiring the partition classes and extend its configurations to {0,1}E∞ by setting all edges outside En closed.

An infinite-volume FK state at (p,q) is any probability measure on {0,1}E∞ that is a cylinder-probability limit of such extended finite-volume laws along a sequence nj→∞ and boundary partitions ξnj. Cylinder-probability convergence means convergence of the probability of every assignment on every finite set of edges. When they exist, the free FK state and wired FK state are the cylinder limits for the identity and one-class partitions, respectively, at every n. Their existence and uniqueness as probability-measure cylinder limits are established by a later A-page lemma under its stated measure-extension hypothesis. For either state ϕp,qb, b∈{0,1}, define θb(p,q):=ϕp,qb(0↔∞), where 0↔∞ means that the open cluster of the origin is not contained in any finite box, and define

pcb(q):=inf⁡{p∈(0,1):θb(p,q)>0}.

No equality of free and wired states at p=pc is part of this definition.

Depends on

Dependency tree · 2 levels

Sources