Encyclopedia Foundation Foundation Pair Kernel Bounded Coupling Mean Field Weight Not Finite Range On En

ARTICLE 3 claims 3 theorems

Foundation Pair Kernel Bounded Coupling Mean Field Weight Not Finite Range On En

A machine-checked proof shows that a simple uniform coupling rule cannot describe local interactions in three dimensions, and names exactly what would be needed to fix it.

The mean-field limit

In the Recognition Science framework, a ledger (a discrete record of recognition events) can carry weights on the links between its entries. The mean-field weight is the simplest possible rule: every entry links to every other entry with the same strength. The declaration meanFieldWeight_not_finiteRangeOn_encodedDist3 is a proved theorem stating that this uniform rule cannot be a local rule in three dimensions. Concretely, on a three-dimensional lattice of size L by L by L (with L at least 2), the mean-field weight assigns a nonzero value to pairs of points that are far apart, so it fails the condition of finite range.

Finite range is the formal way of saying that interactions are local: only entries within a small distance of each other can influence each other. The proof works by measuring distance with the standard "city-block" metric on the lattice, where moving one step along any axis counts as distance 1. The theorem shows that the mean-field weight connects points at distance greater than 1, so it cannot be a nearest-neighbor interaction. This is not a surprise: a rule that connects everything to everything is the opposite of a local rule. The value of the theorem is that it is machine-checked, meaning the proof is verified by a computer program that checks every logical step.

The theorem also contrasts with a positive result in the same file. A different weight, called box weight, assigns nonzero values only to nearest neighbors on the lattice. The framework proves that this box weight does satisfy the finite-range condition. So the framework does not claim that locality is impossible; it claims that the specific mean-field rule is not local, while a specific local alternative exists.

What the theorem does not claim is broader. It does not prove that the mean-field weight is the only non-local rule, nor that locality is forced by the framework's basic assumptions. The framework's basic structure plus a valid tick (a single recognition event) can coexist with weights that are not local at all. The theorem only states a fact about one particular weight on one particular geometry. The framework also does not claim that the box weight is the physically correct rule; that remains an open question, named in the file as ProductionLatticeCouplingObligation.

The practical consequence is a precise boundary. If the framework is to describe a three-dimensional world with local interactions, the mean-field rule cannot be the production rule. The framework must either find a deeper reason that forces local weights, or commit to a specific local rule like the box weight. The theorem sharpens the question: it says where the open problem lies, without pretending to solve it.

THEOREM meanFieldWeight_not_finiteRangeOn_encodedDist3 · IndisputableMonolith/Foundation/PairKernelBoundedCoupling.lean
meanFieldWeight_not_finiteRangeOn_encodedDist3 · IndisputableMonolith/Foundation/PairKernelBoundedCoupling.lean:200
theorem meanFieldWeight_not_finiteRangeOn_encodedDist3
    (L : ℕ) (hL : 2 ≤ L) :
    ¬ FiniteRangeOn (meanFieldWeight (L * L * L)) (encodedDist3 L) 1 := by
  intro hFR
  -- Two axis steps (still available at L = 2) give encodedDist3 = 2 > 1.
  set o : Site3 L := ((⟨0, by omega⟩, ⟨0, by omega⟩), ⟨0, by omega⟩)
  set e : Site3 L := ((⟨1, by omega⟩, ⟨1, by omega⟩), ⟨0, by omega⟩)
  have hdist : encodedDist3 L (enc3 L o) (enc3 L e) = 2 := by
    simp [encodedDist3, Equiv.symm_apply_apply, dist3, Nat.dist, o, e]
  have hfar : 1 < encodedDist3 L (enc3 L o) (enc3 L e) := by
    rw [hdist]
    norm_num
  have hz := hFR (enc3 L o) (enc3 L e) hfar
  simp only [meanFieldWeight] at hz
  exact one_ne_zero hz
THEOREM boxWeight_finiteRangeOn · IndisputableMonolith/Foundation/PairKernelBoundedCoupling.lean
/-- Direct form: `boxWeight` is finite-range in the encoded ℓ¹ metric. -/
theorem boxWeight_finiteRangeOn (L : ℕ) :
    FiniteRangeOn (boxWeight L) (encodedDist3 L) 1 :=
  (boxWeight_finiteRangeOn_export_v1 L).2.2
THEOREM BoundedRecognitionCouplingObligation_not_forced_by_bare_RS · IndisputableMonolith/Foundation/PairKernelBoundedCoupling.lean
BoundedRecognitionCouplingObligation_not_forced_by_bare_RS · IndisputableMonolith/Foundation/PairKernelBoundedCoupling.lean:90
/-- Bundle alias matching the named season obligation string. -/
theorem BoundedRecognitionCouplingObligation_not_forced_by_bare_RS
    (radius : ℕ) :
    ∃ n : ℕ,
      Nonempty (AtomicTick (tickCarrier n)) ∧
        ¬ BoundedRecognitionRelation (tickCarrier n).R radius ∧
          ¬ FiniteRange (meanFieldWeight n) radius := by
  rcases recognitionStructure_atomicTick_do_not_force_boundedCoupling radius with
    ⟨n, hTick, hB, _hS, hFR⟩
  exact ⟨n, hTick, hB, hFR⟩

What this page does not claim

The mean-field weight is the only non-local weight; the theorem concerns one specific weight. Locality is forced by the framework's basic assumptions; the theorem shows the opposite. The box weight is the physically correct rule; it is a committed geometry, not a derived one.

Verify this page

Every tagged claim above names its theorem. To check one yourself rather than trust this page, elaborate the source module with Lean 4 and audit its axiom basis:

$ lake env lean IndisputableMonolith/Foundation/PairKernelBoundedCoupling.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)

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