Encyclopedia Foundation Foundation Dalembert Inevitability Axiom Bundle Necessary

ARTICLE 2 claims 2 theorems

Foundation Dalembert Inevitability Axiom Bundle Necessary

A single equation governs how any consistent cost function must combine, and the proof shows it is the only possible form.

The forced ledger

The d'Alembert functional equation, named for Jean le Rond d'Alembert's 1747 work on vibrating strings, is a classical relation that asks how a function behaves when its arguments are multiplied and divided. For a function F defined on positive numbers, the equation takes the form F(xy) + F(x/y) = 2F(x)F(y) + 2F(x) + 2F(y). Its solutions, under mild regularity conditions, are familiar trigonometric and hyperbolic functions. The equation appears across mathematics, from harmonic analysis to probability, wherever a quantity must combine consistently under scaling.

In Recognition Science, the same equation emerges from a different starting point. The framework models a ledger, a discrete record of comparison events, and asks what cost function F(x) must look like if it measures the cost of a deviation from unity. Three plain conditions are imposed: symmetry (F(x) = F(1/x), so swapping a ratio for its reciprocal costs the same), normalization (F(1) = 0, so no deviation costs nothing), and multiplicative consistency (the cost of a product and a quotient combine through a fixed polynomial P). The framework's machine-checked library of formal theorems proves that any cost function meeting these conditions, together with continuity and non-triviality, forces the combining polynomial to have the unique bilinear form P(u, v) = 2u + 2v + c·uv for some constant c. The proof is a theorem in the library, verified by a computer, and it does not rely on any framework-specific axiom beyond the standard logical postulates of the ambient type theory.

The result is packaged in a declaration named axiom_bundle_necessary. It states three facts together: normalization is definitional, the bilinear family is forced, and a calibration condition F''(1) = 1 fixes the scale. The declaration does not prove that the constant c must equal 2; that choice is a normalization of units, not a forced consequence. It also does not prove that the full cost function J(x) = (x + 1/x)/2 - 1 is the unique solution to the d'Alembert equation, because the theorem only pins the polynomial P, not the function F itself. The uniqueness of J is a separate result in the framework, proved elsewhere, and it depends on the same regularity and non-triviality assumptions.

What the declaration establishes is narrower but still substantial: within the framework's model, the polynomial that combines costs is not arbitrary. Any symmetric, normalized, multiplicatively consistent cost function must use a bilinear combiner. That conclusion is what makes the later derivation of the golden ratio and the eight-tick cycle possible. The reader can now see that the framework's axioms are not a free choice; they are the only polynomial form that survives the consistency requirement.

THEOREM bilinear_family_forced · IndisputableMonolith/Foundation/DAlembert/Inevitability.lean
/-- **THEOREM: The consistency requirement forces the unique bilinear family.**

Given:
1. F : ℝ₊ → ℝ is a cost functional
2. F is symmetric: F(x) = F(1/x)
3. F is normalized: F(1) = 0
4. F has multiplicative consistency: F(xy) + F(x/y) = P(F(x), F(y)) for some **symmetric quadratic polynomial** P
5. F is non-trivial (not constant 0)

Then:
P(u, v) = 2u + 2v + c*u*v for some constant c.

This means F satisfies the generalized d'Alembert equation.
If we choose the canonical cost normalization c = 2, we recover the RCL. -/
theorem bilinear_family_forced (F : ℝ → ℝ) (P : ℝ → ℝ → ℝ)
    (hNorm : IsNormalized F)
    (hCons : HasMultiplicativeConsistency F P)
    (hPoly : ∃ (a b c d e f : ℝ), ∀ u v, P u v = a + b*u + c*v + d*u*v + e*u^2 + f*v^2)
    (hSymP : ∀ u v, P u v = P v u) -- Explicit symmetry of P
    (hNonTriv : ∃ x : ℝ, 0 < x ∧ F x ≠ 0)
    (hCont : ContinuousOn F (Set.Ioi 0)) -- Regularity: F is continuous on (0, ∞)
    : ∃ c : ℝ, (∀ u v, P u v = 2*u + 2*v + c*u*v) ∧
               (c = 2 → ∀ u v, P u v = 2*u + 2*v + 2*u*v) := by
  -- Derived reciprocity from symmetry of P
  have hSym : IsSymmetric F := F_symmetric_of_P_symmetric F P hCons hSymP
  -- Step 1: Normalization forces P(0, v) = 2v
  have hP0 : ∀ y : ℝ, 0 < y → P 0 (F y) = 2 * F y :=
    symmetry_and_normalization_constrain_P F P hSym hNorm hCons

  -- Use the polynomial form lemma
  -- We need to satisfy the hypotheses of `polynomial_form_forced`.
  -- `hNorm0`: ∀ v, P 0 v = 2 * v.
  -- We only have `P 0 (F y) = 2 F y`.
  -- However, since P is a polynomial and F is non-trivial (has range with at least 0 and some non-zero value),
  -- we can determine the coefficients.
  -- P(0, v) = a + c*v + f*v^2.
  -- P(0, 0) = a = 2*0 = 0 (from F(1)=0).
  -- P(0, F y) = c*(F y) + f*(F y)^2 = 2*(F y).
  -- This holds for y=1 (0=0) and some y where F y ≠ 0.
  -- If we only have two points, we can't uniquely determine a quadratic.
  -- But wait, `polynomial_form_forced` derived `a=0, c=2, f=0`.
  -- Let's reproduce that logic but being careful about the domain.

  obtain ⟨a, b, c, d, e, f, hP⟩ := hPoly

  -- 1. a = 0
  have ha : a = 0 := by
    have hCons1 := hCons 1 1 one_pos one_pos
    simp only [one_mul, one_div] at hCons1
    -- hCons1 : F 1 + F 1⁻¹ = P (F 1) (F 1)
    -- inv_one : 1⁻¹ = 1
    rw [inv_one, hNorm] at hCons1
    -- hCons1 : 0 + 0 = P 0 0
    simp only [add_zero] at hCons1
    -- hCons1 : 0 = P 0 0
    rw [hP 0 0] at hCons1
    simp at hCons1
    exact hCons1.symm

  -- 2. From hSymP: P(u,v) = P(v,u)
  -- a + bu + cv + duv + eu^2 + fv^2 = a + bv + cu + duv + ev^2 + fu^2
  -- (b-c)u + (c-b)v + (e-f)u^2 + (f-e)v^2 = 0
  -- This implies b=c and e=f.
  have hb_c : b = c := by
    have h1 := hSymP 1 0
    rw [hP 1 0, hP 0 1] at h1
    -- h1 : a + b*1 + c*0 + d*0 + e*1 + f*0 = a + b*0 + c*1 + d*0 + e*0 + f*1
    -- i.e., a + b + e = a + c + f
    -- Using ha: a = 0, we get b + e = c + f
    simp only [ha, mul_zero, mul_one, add_zero, zero_add] at h1
    -- We need another equation to separate b, e, c, f
    have h2 := hSymP 2 0
    rw [hP 2 0, hP 0 2] at h2
    simp only [ha, mul_zero, add_zero, zero_add] at h2
    -- h1: b + e = c + f
    -- h2: 2b + 4e = 2c + 4f
    -- From h2: b + 2e = c + 2f
    -- Subtracting h1: e = f
    -- So b = c
    linarith
  have he_f : e = f := by
    have h1 := hSymP 1 0
    have h2 := hSymP 2 0
    rw [hP 1 0, hP 0 1] at h1
    rw [hP 2 0, hP 0 2] at h2
    simp only [ha, mul_zero, mul_one, add_zero, zero_add] at h1 h2
    linarith

  -- Now P(0, v) = c*v + f*v^2 (using a=0, b=c, e=f).
  -- And P(0, F y) = 2 * F y.
  -- So c*(F y) + f*(F y)^2 = 2*(F y).
  -- (c - 2)*(F y) + f*(F y)^2 = 0.
  -- This must hold for all y > 0.
  -- Since F is non-trivial, there exists y such that F y ≠ 0.
  obtain ⟨y0, hy0_pos, hy0_ne⟩ := hNonTriv
  have hc_2 : c = 2 ∧ f = 0 := by
    -- Let k = F y0 (a nonzero value in the range).
    let k : ℝ := F y0
    have hk_ne : k ≠ 0 := by
      -- hy0_ne : F y0 ≠ 0
      simpa [k] using hy0_ne

    -- The polynomial identity on the range: (c - 2) * F(y) + f * (F(y))^2 = 0.
    have poly_identity : ∀ y : ℝ, 0 < y → (c - 2) * (F y) + f * (F y)^2 = 0 := by
      intro y hy
      have h := hP0 y hy
      rw [hP 0 (F y)] at h
      simp [ha, hb_c, he_f] at h
      linarith

    -- Use IVT to find y1 with F y1 = k/2 (since F(1)=0 and F(y0)=k).
    have hF1 : F 1 = 0 := hNorm
    have hInterval_pos : Set.uIcc 1 y0 ⊆ Set.Ioi 0 := by
      intro x hx
      rcases hx with ⟨hx_lo, _hx_hi⟩
      have hmin_pos : 0 < min 1 y0 := lt_min one_pos hy0_pos
      exact lt_of_lt_of_le hmin_pos hx_lo
    have hContInterval : ContinuousOn F (Set.uIcc 1 y0) :=
      hCont.mono hInterval_pos
    have h1_mem : 1 ∈ Set.uIcc 1 y0 := Set.left_mem_uIcc
    have hy0_mem : y0 ∈ Set.uIcc 1 y0 := Set.right_mem_uIcc
    have hk2_in_image : k / 2 ∈ F '' Set.uIcc 1 y0 := by
      have hPreconn := isPreconnected_uIcc (a := 1) (b := y0)
      by_cases hk : 0 ≤ k
      · -- monotone direction: 0 ≤ k, so k/2 ∈ Icc 0 k
        have hIVT : Set.Icc 0 k ⊆ F '' Set.uIcc 1 y0 := by
          simpa [hF1, k] using hPreconn.intermediate_value h1_mem hy0_mem hContInterval
        have hk2_between : k / 2 ∈ Set.Icc 0 k := by
          constructor <;> linarith
        exact hIVT hk2_between
      · -- reverse direction: k < 0, so k/2 ∈ Icc k 0
        have hk_lt : k < 0 := lt_of_not_ge hk
        have hIVT : Set.Icc k 0 ⊆ F '' Set.uIcc 1 y0 := by
          simpa [hF1, k] using hPreconn.intermediate_value hy0_mem h1_mem hContInterval
        have hk2_between : k / 2 ∈ Set.Icc k 0 := by
          constructor <;> linarith
        exact hIVT hk2_between
    obtain ⟨y1, hy1_mem, hFy1⟩ := hk2_in_image
    have hy1_pos : 0 < y1 := hInterval_pos hy1_mem

    -- Evaluate the polynomial identity at y0 and y1, then solve for c and f.
    have h_y0 : (c - 2) * k + f * k^2 = 0 := by
      have h := poly_identity y0 hy0_pos
      simpa [k] using h
    have h_y1 : (c - 2) * (k / 2) + f * (k / 2)^2 = 0 := by
      have h := poly_identity y1 hy1_pos
      -- rewrite F y1 = k/2
      simpa [hFy1, k] using h

    -- Multiply the y1 equation by 4 to align it with the y0 equation.
    have h_y1_4 : 2 * (c - 2) * k + f * k^2 = 0 := by
      have h' := congrArg (fun z => 4 * z) h_y1
      -- simplify 4*(...) and 4*0
      ring_nf at h'
      -- `ring_nf` chooses its own normal form; bridge to our preferred one.
      have hrew : c * k * 2 - k * 4 + k ^ 2 * f = 2 * (c - 2) * k + f * k ^ 2 := by ring
      -- h' : c*k*2 - k*4 + k^2*f = 0
      calc
        2 * (c - 2) * k + f * k ^ 2
            = c * k * 2 - k * 4 + k ^ 2 * f := by simpa [hrew] using (Eq.symm hrew)
        _ = 0 := h'

    -- Subtract to get (c - 2) * k = 0, hence c = 2 (since k ≠ 0).
    have hk_mul : (c - 2) * k = 0 := by
      linarith [h_y0, h_y1_4]
    have hc : c = 2 := by
      rcases mul_eq_zero.mp hk_mul with hc0 | hk0
      · linarith
      · exact False.elim (hk_ne hk0)

    -- Plug back to get f = 0.
    have hf : f = 0 := by
      have hk2_ne : k^2 ≠ 0 := pow_ne_zero 2 hk_ne
      have hfk2 : f * k^2 = 0 := by
        -- from h_y0 with c=2
        simpa [hc] using h_y0
      rcases mul_eq_zero.mp hfk2 with hf0 | hk20
      · exact hf0
      · exact False.elim (hk2_ne hk20)

    exact ⟨hc, hf⟩

  have hc : c = 2 := hc_2.1
  have hf : f = 0 := hc_2.2
  have hb : b = 2 := by rw [hb_c, hc]
  have he : e = 0 := by rw [he_f, hf]

  -- So P(u, v) = 2u + 2v + d*u*v.
  use d
  constructor
  · intro u v
    rw [hP, ha, hb, hc, he, hf]
    ring
  · intro hd u v
    rw [hP, ha, hb, hc, he, hf, hd]
    ring
THEOREM axiom_bundle_necessary · IndisputableMonolith/Foundation/DAlembert/Inevitability.lean
/-- **COROLLARY: The Recognition Science axiom bundle (A1, A2, A3) is transcendentally necessary.**

- A1 (Normalization): F(1) = 0
  → Definitional for "cost of deviation from unity"

- A2 (RCL): F(xy) + F(x/y) = 2F(x)F(y) + 2F(x) + 2F(y)
  → PROVED: The unique polynomial form for multiplicative consistency (up to scale)

- A3 (Calibration): F''(1) = 1
  → Sets the natural scale (removes family degeneracy)

Therefore: The entire axiom bundle is not arbitrary but forced by the structure of comparison. -/
theorem axiom_bundle_necessary :
    -- A1: Normalization is definitional
    (∀ F : ℝ → ℝ, (∀ x : ℝ, 0 < x → F x = Cost.Jcost x) → F 1 = 0) ∧
    -- A2: RCL is the unique polynomial form (proven above)
    (∀ F P, IsNormalized F → HasMultiplicativeConsistency F P →
      (∃ a b c d e f, ∀ u v, P u v = a + b*u + c*v + d*u*v + e*u^2 + f*v^2) →
      (∀ u v, P u v = P v u) → -- Symmetry requirement
      (∃ x, 0 < x ∧ F x ≠ 0) → -- Non-triviality
      ContinuousOn F (Set.Ioi 0) → -- Regularity
      ∃ c, ∀ u v, P u v = 2*u + 2*v + c*u*v) ∧
    -- A3: Calibration pins down the scale (J''(1) = 1)
    (deriv (deriv (fun x => Cost.Jcost x)) 1 = 1) := by
  constructor
  · intro F hF
    have h := hF 1 one_pos
    simp only [Cost.Jcost, inv_one] at h
    linarith
  constructor
  · intro F P hNorm hCons hPoly hSymP hNonTriv hCont
    -- Use bilinear_family_forced and extract the first conjunct
    obtain ⟨c, hc, _⟩ := bilinear_family_forced F P hNorm hCons hPoly hSymP hNonTriv hCont
    exact ⟨c, hc⟩
  · -- Prove J''(1) = 1 (calibration)
    -- J(x) = x/2 + 1/(2x) - 1, so J''(x) = x⁻³, thus J''(1) = 1.
    exact Cost.deriv2_Jcost_one

What this page does not claim

The theorem does not force the constant c to equal 2; that is a unit normalization. The theorem does not prove uniqueness of the cost function J itself, only the polynomial combiner. The proof does not rely on any framework-specific axiom beyond standard logical postulates.

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/DAlembert/Inevitability.lean
expected axiom basis: [propext, Classical.choice, Quot.sound] (the Lean kernel's standard three; no RS-specific axioms)

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