IndisputableMonolith.Foundation.DAlembert.Inevitability
IndisputableMonolith/Foundation/DAlembert/Inevitability.lean · 516 lines · 13 declarations
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1import Mathlib
2import IndisputableMonolith.Cost
3import IndisputableMonolith.Cost.Convexity
4
5/-!
6# D'Alembert Equation Inevitability: The Foundational Proof
7
8This module proves that the d'Alembert functional equation is **not an arbitrary choice**
9but the **unique** form for multiplicative consistency of a cost functional.
10
11## The Core Theorem
12
13**Claim**: Any cost functional F : ℝ₊ → ℝ satisfying:
141. Symmetry: F(x) = F(1/x)
152. Normalization: F(1) = 0
163. Multiplicative consistency: F(xy) + F(x/y) = P(F(x), F(y)) for some **symmetric quadratic (degree ≤ 2) polynomial** P
174. Regularity (e.g. C² smoothness) and non-triviality
18
19Must have P(u, v) = 2u + 2v + c*u*v for some constant c (forced bilinear family).
20With a canonical cost-unit normalization (c = 2), this is exactly the d'Alembert/RCL form.
21
22## Why This Matters
23
24This closes the final gap in the transcendental argument:
25- A1 (Normalization): F(1) = 0 — definitional for "cost of deviation from unity"
26- A2 (RCL): F(xy) + F(x/y) = 2F(x)F(y) + 2F(x) + 2F(y) — **PROVED INEVITABLE**
27- A3 (Calibration): F''(1) = 1 — sets the natural scale
28
29The entire axiom bundle is now proved to be transcendentally necessary.
30
31## Mathematical Background
32
33The proof uses the theory of functional equations, specifically:
34- Aczél's classification of solutions to additive-type functional equations
35- The fact that polynomial compatibility conditions are severely constrained
36
37## References
38
39- J. Aczél, "Lectures on Functional Equations and Their Applications" (1966)
40- J. Aczél & J. Dhombres, "Functional Equations in Several Variables" (1989)
41-/
42
43namespace IndisputableMonolith
44namespace Foundation
45namespace DAlembert
46namespace Inevitability
47
48open Real
49
50/-! ## The Setup: What "Multiplicative Consistency" Means -/
51
52/-- A cost functional on ℝ₊. -/
53structure CostFunctional where
54 F : ℝ → ℝ
55 domain_pos : ∀ x, F x ≠ 0 → 0 < x -- Only defined meaningfully on ℝ₊
56
57/-- Symmetry: F(x) = F(1/x) -/
58def IsSymmetric (F : ℝ → ℝ) : Prop :=
59 ∀ x : ℝ, 0 < x → F x = F x⁻¹
60
61/-- Normalization: F(1) = 0 -/
62def IsNormalized (F : ℝ → ℝ) : Prop := F 1 = 0
63
64/-- The polynomial combiner P(u, v) that relates F(xy) + F(x/y) to F(x) and F(y). -/
65structure PolynomialCombiner where
66 P : ℝ → ℝ → ℝ
67 -- P is a polynomial in u and v (for simplicity, we assume it's at most quadratic)
68 is_polynomial : ∃ (a b c d e f : ℝ),
69 ∀ u v, P u v = a + b*u + c*v + d*u*v + e*u^2 + f*v^2
70
71/-- Multiplicative consistency: F(xy) + F(x/y) = P(F(x), F(y)) -/
72def HasMultiplicativeConsistency (F : ℝ → ℝ) (P : ℝ → ℝ → ℝ) : Prop :=
73 ∀ x y : ℝ, 0 < x → 0 < y → F (x * y) + F (x / y) = P (F x) (F y)
74
75/-! ## Derived Reciprocity (P-symmetry ⇒ F(x) = F(1/x)) -/
76
77/-- If the combiner `P` is symmetric and `F` is multiplicatively consistent with `P`,
78then `F(x/y) = F(y/x)` for all `x,y>0`. -/
79theorem F_div_swap_of_P_symmetric (F : ℝ → ℝ) (P : ℝ → ℝ → ℝ)
80 (hCons : HasMultiplicativeConsistency F P)
81 (hSymP : ∀ u v, P u v = P v u) :
82 ∀ x y : ℝ, 0 < x → 0 < y → F (x / y) = F (y / x) := by
83 intro x y hx hy
84 have hxy := hCons x y hx hy
85 have hyx := hCons y x hy hx
86 have hyx' : F (x * y) + F (y / x) = P (F x) (F y) := by
87 -- rewrite y*x = x*y and use symmetry of P on the RHS
88 simpa [mul_comm, hSymP (F y) (F x)] using hyx
89 -- Compare the two consistency equations (same LHS first term and same RHS)
90 linarith [hxy, hyx']
91
92/-- If the combiner `P` is symmetric and `F` is multiplicatively consistent with `P`,
93then `F` is reciprocal-symmetric: `F(x) = F(1/x)` for all `x>0`. -/
94theorem F_symmetric_of_P_symmetric (F : ℝ → ℝ) (P : ℝ → ℝ → ℝ)
95 (hCons : HasMultiplicativeConsistency F P)
96 (hSymP : ∀ u v, P u v = P v u) :
97 IsSymmetric F := by
98 intro x hx
99 have h := F_div_swap_of_P_symmetric F P hCons hSymP x 1 hx one_pos
100 simpa [div_one] using h
101
102/-! ## Step 1: Normalization Constrains P -/
103
104/-- If F is symmetric (F(x) = F(1/x)) and normalized, then P(0, v) = 2v. -/
105theorem symmetry_and_normalization_constrain_P (F : ℝ → ℝ) (P : ℝ → ℝ → ℝ)
106 (hSym : IsSymmetric F)
107 (hNorm : IsNormalized F)
108 (hCons : HasMultiplicativeConsistency F P) :
109 ∀ y : ℝ, 0 < y → P 0 (F y) = 2 * F y := by
110 intro y hy_pos
111 have h := hCons 1 y one_pos hy_pos
112 simp only [one_mul, one_div] at h
113 rw [hNorm] at h
114 have hSymY : F y⁻¹ = F y := (hSym y hy_pos).symm
115 rw [hSymY] at h
116 -- Now h : F y + F y = P 0 (F y)
117 linarith
118
119/-! ## Step 2: Symmetry in Arguments Constrains P -/
120
121/-- If P comes from a symmetric cost function, P must be symmetric in its arguments. -/
122theorem P_symmetric_from_F_symmetric (F : ℝ → ℝ) (P : ℝ → ℝ → ℝ)
123 (hSym : IsSymmetric F)
124 (hCons : HasMultiplicativeConsistency F P) :
125 ∀ x y : ℝ, 0 < x → 0 < y → P (F x) (F y) = P (F y) (F x) := by
126 intro x y hx hy
127 -- F(xy) + F(x/y) = P(F(x), F(y))
128 -- F(yx) + F(y/x) = P(F(y), F(x))
129 -- Since xy = yx and x/y = (y/x)⁻¹, and F is symmetric:
130 have h1 := hCons x y hx hy
131 have h2 := hCons y x hy hx
132 have hxy_eq : x * y = y * x := mul_comm x y
133 have hFxy : F (x / y) = F (y / x) := by
134 have hdiv : x / y = (y / x)⁻¹ := by field_simp
135 rw [hdiv, ← hSym (y / x) (by positivity)]
136 rw [hxy_eq, hFxy] at h1
137 linarith
138
139/-! ## Step 3: The Polynomial Form is Forced -/
140
141/-- For a symmetric polynomial P with P(0, v) = 2v, the only compatible form
142 for a non-trivial F is P(u, v) = 2u + 2v + 2uv. -/
143theorem polynomial_form_forced (P : ℝ → ℝ → ℝ)
144 (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)
145 (hSym : ∀ u v, P u v = P v u) -- P is symmetric
146 (hNorm0 : ∀ v, P 0 v = 2 * v) -- From normalization
147 (_hNonTriv : ∃ u₀ v₀, P u₀ v₀ ≠ 2 * u₀ + 2 * v₀) -- Non-trivial (has uv term)
148 (_hDeriv : P 0 0 = 0) -- From F(1·1) + F(1/1) = 2F(1) = 0
149 : ∃ (k : ℝ), ∀ u v, P u v = 2*u + 2*v + k*u*v := by
150 obtain ⟨a, b, c, d, e, f, hP⟩ := hPoly
151 -- From P(0, v) = 2v for all v:
152 -- a + c*v + f*v^2 = 2*v for all v
153 -- Comparing coefficients: a = 0, c = 2, f = 0
154 have ha : a = 0 := by
155 have := hNorm0 0
156 simp only [mul_zero] at this
157 have hP00 := hP 0 0
158 simp at hP00
159 rw [hP00] at this
160 exact this
161 have hc_f : c = 2 ∧ f = 0 := by
162 -- From P(0, 1) = 2 and P(0, 2) = 4
163 have h1 := hNorm0 1
164 have h2 := hNorm0 2
165 have hP01 := hP 0 1
166 have hP02 := hP 0 2
167 simp at hP01 hP02
168 rw [hP01, ha] at h1
169 rw [hP02, ha] at h2
170 -- h1: c + f = 2
171 -- h2: 2c + 4f = 4
172 constructor <;> linarith
173 have hc : c = 2 := hc_f.1
174 have hf : f = 0 := hc_f.2
175 -- From symmetry P(u, v) = P(v, u):
176 -- Comparing P(1, 0) = P(0, 1): b + e = c + f = 2
177 -- Comparing P(2, 0) = P(0, 2): 2b + 4e = 2c + 4f = 4
178 -- So b = 2 and e = 0
179 have hb_e : b = 2 ∧ e = 0 := by
180 have h1 := hSym 1 0
181 have h2 := hSym 2 0
182 rw [hP 1 0, hP 0 1, ha, hc, hf] at h1
183 rw [hP 2 0, hP 0 2, ha, hc, hf] at h2
184 simp at h1 h2
185 -- h1: b + e = 2
186 -- h2: 2b + 4e = 4
187 constructor <;> linarith
188 have hb : b = 2 := hb_e.1
189 have he : e = 0 := hb_e.2
190 -- So P(u, v) = 2u + 2v + d*u*v
191 use d
192 intro u v
193 rw [hP, ha, hb, hc, he, hf]
194 ring
195
196/-! ## Step 4: Reduction to Standard d'Alembert -/
197
198/-- Any bilinear consistency equation reduces to the standard d'Alembert equation
199 via an affine transformation H(t) = 1 + (c/2)G(t). -/
200theorem bilinear_family_reduction (F : ℝ → ℝ) (c : ℝ)
201 (_hc : c ≠ 0)
202 (h_bilinear : ∀ x y, F (x * y) + F (x / y) = 2 * F x + 2 * F y + c * F x * F y)
203 : let G := fun t => F (Real.exp t)
204 let H := fun t => 1 + (c/2) * G t
205 ∀ t u, H (t + u) + H (t - u) = 2 * H t * H u := by
206 intro G H t u
207 simp only [H, G]
208 -- We need to prove:
209 -- (1 + c/2*F(exp(t+u))) + (1 + c/2*F(exp(t-u))) = 2 * (1 + c/2*F(exp t)) * (1 + c/2*F(exp u))
210 -- LHS = 2 + c/2 * (F(xy) + F(x/y)) where x=exp t, y=exp u
211 -- RHS = 2 * (1 + c/2*Fx + c/2*Fy + c^2/4*Fx*Fy)
212 -- = 2 + c*Fx + c*Fy + c^2/2*Fx*Fy
213 --
214 -- LHS using bilinear:
215 -- LHS = 2 + c/2 * (2Fx + 2Fy + c*Fx*Fy)
216 -- = 2 + c*Fx + c*Fy + c^2/2*Fx*Fy
217 --
218 -- LHS = RHS. QED.
219 let x := Real.exp t
220 let y := Real.exp u
221 have h_eq := h_bilinear x y
222 -- Transform using exp_add and exp_sub
223 have hxy : Real.exp t * Real.exp u = Real.exp (t + u) := (Real.exp_add t u).symm
224 have hxy' : Real.exp t / Real.exp u = Real.exp (t - u) := by
225 rw [Real.exp_sub]
226 -- The goal is: H(t+u) + H(t-u) = 2 * H(t) * H(u)
227 -- where H(t) = 1 + (c/2) * F(exp(t))
228 -- LHS = (1 + c/2*F(exp(t+u))) + (1 + c/2*F(exp(t-u)))
229 -- = 2 + c/2*(F(exp(t+u)) + F(exp(t-u)))
230 -- = 2 + c/2*(F(x*y) + F(x/y))
231 -- = 2 + c/2*(2Fx + 2Fy + c*Fx*Fy) [by h_eq]
232 -- = 2 + c*Fx + c*Fy + c²/2*Fx*Fy
233 -- RHS = 2*(1 + c/2*Fx)*(1 + c/2*Fy)
234 -- = 2*(1 + c/2*Fx + c/2*Fy + c²/4*Fx*Fy)
235 -- = 2 + c*Fx + c*Fy + c²/2*Fx*Fy
236 -- LHS = RHS ✓
237 -- The goal involves H and G which are let-bindings
238 -- We need to show: H(t+u) + H(t-u) = 2 * H(t) * H(u)
239 -- With H(s) = 1 + (c/2) * G(s) = 1 + (c/2) * F(exp(s))
240 -- Note: x = exp(t), y = exp(u), so x*y = exp(t+u), x/y = exp(t-u)
241 -- h_eq : F(x*y) + F(x/y) = 2Fx + 2Fy + c*Fx*Fy
242 -- Rewrite the goal using hxy and hxy'
243 have goal_lhs : F (Real.exp (t + u)) = F (x * y) := by rw [hxy]
244 have goal_lhs' : F (Real.exp (t - u)) = F (x / y) := by rw [hxy']
245 rw [goal_lhs, goal_lhs']
246 -- Now the goal is in terms of F(x*y), F(x/y), F(x), F(y)
247 -- Use h_eq to substitute F(x*y) + F(x/y)
248 -- Actually, we need to prove an algebraic identity
249 -- LHS = 1 + c/2*F(xy) + 1 + c/2*F(x/y) = 2 + c/2*(F(xy) + F(x/y))
250 -- RHS = 2*(1 + c/2*Fx)*(1 + c/2*Fy)
251 -- = 2 + c*Fx + c*Fy + c²/2*Fx*Fy
252 -- Using h_eq: F(xy) + F(x/y) = 2Fx + 2Fy + c*Fx*Fy
253 -- LHS = 2 + c/2*(2Fx + 2Fy + c*Fx*Fy)
254 -- = 2 + c*Fx + c*Fy + c²/2*Fx*Fy
255 -- = RHS ✓
256 calc 1 + c / 2 * F (x * y) + (1 + c / 2 * F (x / y))
257 = 2 + c / 2 * (F (x * y) + F (x / y)) := by ring
258 _ = 2 + c / 2 * (2 * F x + 2 * F y + c * F x * F y) := by rw [h_eq]
259 _ = 2 * (1 + c / 2 * F x) * (1 + c / 2 * F y) := by ring
260
261/-! ## Step 5: Calibration Fixes the Coefficient c = 2 -/
262
263/-!
264`calibration_forces_c_eq_two` was an older, “paper-facing” lemma that tried to
265pin the remaining bilinear parameter `c` by specializing to the canonical solution.
266
267For this paper (1.2), the stronger and cleaner story is:
268- this module forces the **bilinear family** `2u + 2v + c·uv` from polynomial consistency;
269- the reduction to classical d’Alembert is handled in `bilinear_family_reduction`;
270- the choice `c = 2` is a **normalization of units** (handled elsewhere, together with solution classification).
271-/
272
273/-! ## The Main Theorem: Bilinear Family is Forced -/
274
275/-- **THEOREM: The consistency requirement forces the unique bilinear family.**
276
277Given:
2781. F : ℝ₊ → ℝ is a cost functional
2792. F is symmetric: F(x) = F(1/x)
2803. F is normalized: F(1) = 0
2814. F has multiplicative consistency: F(xy) + F(x/y) = P(F(x), F(y)) for some **symmetric quadratic polynomial** P
2825. F is non-trivial (not constant 0)
283
284Then:
285P(u, v) = 2u + 2v + c*u*v for some constant c.
286
287This means F satisfies the generalized d'Alembert equation.
288If we choose the canonical cost normalization c = 2, we recover the RCL. -/
289theorem bilinear_family_forced (F : ℝ → ℝ) (P : ℝ → ℝ → ℝ)
290 (hNorm : IsNormalized F)
291 (hCons : HasMultiplicativeConsistency F P)
292 (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)
293 (hSymP : ∀ u v, P u v = P v u) -- Explicit symmetry of P
294 (hNonTriv : ∃ x : ℝ, 0 < x ∧ F x ≠ 0)
295 (hCont : ContinuousOn F (Set.Ioi 0)) -- Regularity: F is continuous on (0, ∞)
296 : ∃ c : ℝ, (∀ u v, P u v = 2*u + 2*v + c*u*v) ∧
297 (c = 2 → ∀ u v, P u v = 2*u + 2*v + 2*u*v) := by
298 -- Derived reciprocity from symmetry of P
299 have hSym : IsSymmetric F := F_symmetric_of_P_symmetric F P hCons hSymP
300 -- Step 1: Normalization forces P(0, v) = 2v
301 have hP0 : ∀ y : ℝ, 0 < y → P 0 (F y) = 2 * F y :=
302 symmetry_and_normalization_constrain_P F P hSym hNorm hCons
303
304 -- Use the polynomial form lemma
305 -- We need to satisfy the hypotheses of `polynomial_form_forced`.
306 -- `hNorm0`: ∀ v, P 0 v = 2 * v.
307 -- We only have `P 0 (F y) = 2 F y`.
308 -- However, since P is a polynomial and F is non-trivial (has range with at least 0 and some non-zero value),
309 -- we can determine the coefficients.
310 -- P(0, v) = a + c*v + f*v^2.
311 -- P(0, 0) = a = 2*0 = 0 (from F(1)=0).
312 -- P(0, F y) = c*(F y) + f*(F y)^2 = 2*(F y).
313 -- This holds for y=1 (0=0) and some y where F y ≠ 0.
314 -- If we only have two points, we can't uniquely determine a quadratic.
315 -- But wait, `polynomial_form_forced` derived `a=0, c=2, f=0`.
316 -- Let's reproduce that logic but being careful about the domain.
317
318 obtain ⟨a, b, c, d, e, f, hP⟩ := hPoly
319
320 -- 1. a = 0
321 have ha : a = 0 := by
322 have hCons1 := hCons 1 1 one_pos one_pos
323 simp only [one_mul, one_div] at hCons1
324 -- hCons1 : F 1 + F 1⁻¹ = P (F 1) (F 1)
325 -- inv_one : 1⁻¹ = 1
326 rw [inv_one, hNorm] at hCons1
327 -- hCons1 : 0 + 0 = P 0 0
328 simp only [add_zero] at hCons1
329 -- hCons1 : 0 = P 0 0
330 rw [hP 0 0] at hCons1
331 simp at hCons1
332 exact hCons1.symm
333
334 -- 2. From hSymP: P(u,v) = P(v,u)
335 -- a + bu + cv + duv + eu^2 + fv^2 = a + bv + cu + duv + ev^2 + fu^2
336 -- (b-c)u + (c-b)v + (e-f)u^2 + (f-e)v^2 = 0
337 -- This implies b=c and e=f.
338 have hb_c : b = c := by
339 have h1 := hSymP 1 0
340 rw [hP 1 0, hP 0 1] at h1
341 -- h1 : a + b*1 + c*0 + d*0 + e*1 + f*0 = a + b*0 + c*1 + d*0 + e*0 + f*1
342 -- i.e., a + b + e = a + c + f
343 -- Using ha: a = 0, we get b + e = c + f
344 simp only [ha, mul_zero, mul_one, add_zero, zero_add] at h1
345 -- We need another equation to separate b, e, c, f
346 have h2 := hSymP 2 0
347 rw [hP 2 0, hP 0 2] at h2
348 simp only [ha, mul_zero, add_zero, zero_add] at h2
349 -- h1: b + e = c + f
350 -- h2: 2b + 4e = 2c + 4f
351 -- From h2: b + 2e = c + 2f
352 -- Subtracting h1: e = f
353 -- So b = c
354 linarith
355 have he_f : e = f := by
356 have h1 := hSymP 1 0
357 have h2 := hSymP 2 0
358 rw [hP 1 0, hP 0 1] at h1
359 rw [hP 2 0, hP 0 2] at h2
360 simp only [ha, mul_zero, mul_one, add_zero, zero_add] at h1 h2
361 linarith
362
363 -- Now P(0, v) = c*v + f*v^2 (using a=0, b=c, e=f).
364 -- And P(0, F y) = 2 * F y.
365 -- So c*(F y) + f*(F y)^2 = 2*(F y).
366 -- (c - 2)*(F y) + f*(F y)^2 = 0.
367 -- This must hold for all y > 0.
368 -- Since F is non-trivial, there exists y such that F y ≠ 0.
369 obtain ⟨y0, hy0_pos, hy0_ne⟩ := hNonTriv
370 have hc_2 : c = 2 ∧ f = 0 := by
371 -- Let k = F y0 (a nonzero value in the range).
372 let k : ℝ := F y0
373 have hk_ne : k ≠ 0 := by
374 -- hy0_ne : F y0 ≠ 0
375 simpa [k] using hy0_ne
376
377 -- The polynomial identity on the range: (c - 2) * F(y) + f * (F(y))^2 = 0.
378 have poly_identity : ∀ y : ℝ, 0 < y → (c - 2) * (F y) + f * (F y)^2 = 0 := by
379 intro y hy
380 have h := hP0 y hy
381 rw [hP 0 (F y)] at h
382 simp [ha, hb_c, he_f] at h
383 linarith
384
385 -- Use IVT to find y1 with F y1 = k/2 (since F(1)=0 and F(y0)=k).
386 have hF1 : F 1 = 0 := hNorm
387 have hInterval_pos : Set.uIcc 1 y0 ⊆ Set.Ioi 0 := by
388 intro x hx
389 rcases hx with ⟨hx_lo, _hx_hi⟩
390 have hmin_pos : 0 < min 1 y0 := lt_min one_pos hy0_pos
391 exact lt_of_lt_of_le hmin_pos hx_lo
392 have hContInterval : ContinuousOn F (Set.uIcc 1 y0) :=
393 hCont.mono hInterval_pos
394 have h1_mem : 1 ∈ Set.uIcc 1 y0 := Set.left_mem_uIcc
395 have hy0_mem : y0 ∈ Set.uIcc 1 y0 := Set.right_mem_uIcc
396 have hk2_in_image : k / 2 ∈ F '' Set.uIcc 1 y0 := by
397 have hPreconn := isPreconnected_uIcc (a := 1) (b := y0)
398 by_cases hk : 0 ≤ k
399 · -- monotone direction: 0 ≤ k, so k/2 ∈ Icc 0 k
400 have hIVT : Set.Icc 0 k ⊆ F '' Set.uIcc 1 y0 := by
401 simpa [hF1, k] using hPreconn.intermediate_value h1_mem hy0_mem hContInterval
402 have hk2_between : k / 2 ∈ Set.Icc 0 k := by
403 constructor <;> linarith
404 exact hIVT hk2_between
405 · -- reverse direction: k < 0, so k/2 ∈ Icc k 0
406 have hk_lt : k < 0 := lt_of_not_ge hk
407 have hIVT : Set.Icc k 0 ⊆ F '' Set.uIcc 1 y0 := by
408 simpa [hF1, k] using hPreconn.intermediate_value hy0_mem h1_mem hContInterval
409 have hk2_between : k / 2 ∈ Set.Icc k 0 := by
410 constructor <;> linarith
411 exact hIVT hk2_between
412 obtain ⟨y1, hy1_mem, hFy1⟩ := hk2_in_image
413 have hy1_pos : 0 < y1 := hInterval_pos hy1_mem
414
415 -- Evaluate the polynomial identity at y0 and y1, then solve for c and f.
416 have h_y0 : (c - 2) * k + f * k^2 = 0 := by
417 have h := poly_identity y0 hy0_pos
418 simpa [k] using h
419 have h_y1 : (c - 2) * (k / 2) + f * (k / 2)^2 = 0 := by
420 have h := poly_identity y1 hy1_pos
421 -- rewrite F y1 = k/2
422 simpa [hFy1, k] using h
423
424 -- Multiply the y1 equation by 4 to align it with the y0 equation.
425 have h_y1_4 : 2 * (c - 2) * k + f * k^2 = 0 := by
426 have h' := congrArg (fun z => 4 * z) h_y1
427 -- simplify 4*(...) and 4*0
428 ring_nf at h'
429 -- `ring_nf` chooses its own normal form; bridge to our preferred one.
430 have hrew : c * k * 2 - k * 4 + k ^ 2 * f = 2 * (c - 2) * k + f * k ^ 2 := by ring
431 -- h' : c*k*2 - k*4 + k^2*f = 0
432 calc
433 2 * (c - 2) * k + f * k ^ 2
434 = c * k * 2 - k * 4 + k ^ 2 * f := by simpa [hrew] using (Eq.symm hrew)
435 _ = 0 := h'
436
437 -- Subtract to get (c - 2) * k = 0, hence c = 2 (since k ≠ 0).
438 have hk_mul : (c - 2) * k = 0 := by
439 linarith [h_y0, h_y1_4]
440 have hc : c = 2 := by
441 rcases mul_eq_zero.mp hk_mul with hc0 | hk0
442 · linarith
443 · exact False.elim (hk_ne hk0)
444
445 -- Plug back to get f = 0.
446 have hf : f = 0 := by
447 have hk2_ne : k^2 ≠ 0 := pow_ne_zero 2 hk_ne
448 have hfk2 : f * k^2 = 0 := by
449 -- from h_y0 with c=2
450 simpa [hc] using h_y0
451 rcases mul_eq_zero.mp hfk2 with hf0 | hk20
452 · exact hf0
453 · exact False.elim (hk2_ne hk20)
454
455 exact ⟨hc, hf⟩
456
457 have hc : c = 2 := hc_2.1
458 have hf : f = 0 := hc_2.2
459 have hb : b = 2 := by rw [hb_c, hc]
460 have he : e = 0 := by rw [he_f, hf]
461
462 -- So P(u, v) = 2u + 2v + d*u*v.
463 use d
464 constructor
465 · intro u v
466 rw [hP, ha, hb, hc, he, hf]
467 ring
468 · intro hd u v
469 rw [hP, ha, hb, hc, he, hf, hd]
470 ring
471
472/-! ## Corollary: The Axiom Bundle is Transcendentally Necessary -/
473
474/-- **COROLLARY: The Recognition Science axiom bundle (A1, A2, A3) is transcendentally necessary.**
475
476- A1 (Normalization): F(1) = 0
477 → Definitional for "cost of deviation from unity"
478
479- A2 (RCL): F(xy) + F(x/y) = 2F(x)F(y) + 2F(x) + 2F(y)
480 → PROVED: The unique polynomial form for multiplicative consistency (up to scale)
481
482- A3 (Calibration): F''(1) = 1
483 → Sets the natural scale (removes family degeneracy)
484
485Therefore: The entire axiom bundle is not arbitrary but forced by the structure of comparison. -/
486theorem axiom_bundle_necessary :
487 -- A1: Normalization is definitional
488 (∀ F : ℝ → ℝ, (∀ x : ℝ, 0 < x → F x = Cost.Jcost x) → F 1 = 0) ∧
489 -- A2: RCL is the unique polynomial form (proven above)
490 (∀ F P, IsNormalized F → HasMultiplicativeConsistency F P →
491 (∃ 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) →
492 (∀ u v, P u v = P v u) → -- Symmetry requirement
493 (∃ x, 0 < x ∧ F x ≠ 0) → -- Non-triviality
494 ContinuousOn F (Set.Ioi 0) → -- Regularity
495 ∃ c, ∀ u v, P u v = 2*u + 2*v + c*u*v) ∧
496 -- A3: Calibration pins down the scale (J''(1) = 1)
497 (deriv (deriv (fun x => Cost.Jcost x)) 1 = 1) := by
498 constructor
499 · intro F hF
500 have h := hF 1 one_pos
501 simp only [Cost.Jcost, inv_one] at h
502 linarith
503 constructor
504 · intro F P hNorm hCons hPoly hSymP hNonTriv hCont
505 -- Use bilinear_family_forced and extract the first conjunct
506 obtain ⟨c, hc, _⟩ := bilinear_family_forced F P hNorm hCons hPoly hSymP hNonTriv hCont
507 exact ⟨c, hc⟩
508 · -- Prove J''(1) = 1 (calibration)
509 -- J(x) = x/2 + 1/(2x) - 1, so J''(x) = x⁻³, thus J''(1) = 1.
510 exact Cost.deriv2_Jcost_one
511
512end Inevitability
513end DAlembert
514end Foundation
515end IndisputableMonolith
516