IndisputableMonolith.NumberTheory.VectorCSymmetryOnlyNoGo
IndisputableMonolith/NumberTheory/VectorCSymmetryOnlyNoGo.lean · 160 lines · 12 declarations
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1import Mathlib
2import IndisputableMonolith.NumberTheory.CompletedXiSymmetry
3import IndisputableMonolith.NumberTheory.ZeroDoublingLaw
4import IndisputableMonolith.NumberTheory.ZeroCompositionInterface
5
6/-!
7# Vector C Symmetry-Only No-Go
8
9This module formalizes the main stage gate for Vector C:
10
11functional-equation reflection symmetry plus conjugation symmetry give
12pairing data on zeros, but do not by themselves force the critical line.
13
14We certify this with an explicit toy completed-ξ surface whose zeros occur on
15the off-line pair `Re(s) = 1/4, 3/4`.
16-/
17
18namespace IndisputableMonolith
19namespace NumberTheory
20
21open scoped ComplexConjugate
22
23noncomputable section
24
25/-- A toy completed-ξ-style function depending only on the real part.
26
27Its zero set is exactly the union of the two vertical lines `Re(s) = 1/4` and
28`Re(s) = 3/4`, so it satisfies reflection and conjugation symmetry while still
29admitting off-critical-line zeros. -/
30def toyXi (s : ℂ) : ℂ :=
31 Complex.ofReal (((s.re - 3 / 4) ^ 2) * ((s.re - 1 / 4) ^ 2))
32
33theorem toyXi_reflection (s : ℂ) :
34 toyXi (functionalReflection s) = toyXi s := by
35 simp [toyXi, functionalReflection]
36 ring
37
38theorem toyXi_conjugation (s : ℂ) :
39 toyXi (conj s) = conj (toyXi s) := by
40 unfold toyXi
41 rw [Complex.conj_ofReal]
42 have hre : (conj s).re = s.re := by simp
43 rw [hre]
44
45/-- A concrete symmetry surface showing that FE-style pairing data alone does
46not force critical-line support. -/
47def toyCompletedXiSurface : CompletedXiSurface where
48 xi := toyXi
49 reflection := toyXi_reflection
50 conjugation := toyXi_conjugation
51
52/-- The toy surface has a zero at `s = 3/4`. -/
53theorem toyCompletedXiSurface_has_off_critical_zero :
54 toyCompletedXiSurface.xi (3 / 4 : ℂ) = 0 ∧
55 ¬ OnCriticalLine (3 / 4 : ℂ) := by
56 constructor
57 · norm_num [toyCompletedXiSurface, toyXi]
58 · norm_num [OnCriticalLine]
59
60/-- Reflection/conjugation symmetry of the completed-ξ surface alone is
61insufficient to force the critical line. -/
62theorem completedXiSurface_symmetry_only_no_go :
63 ¬ (∀ Ξ : CompletedXiSurface, ∀ s : ℂ, Ξ.xi s = 0 → OnCriticalLine s) := by
64 intro h
65 obtain ⟨hzero, hline⟩ := toyCompletedXiSurface_has_off_critical_zero
66 exact hline (h toyCompletedXiSurface (3 / 4 : ℂ) hzero)
67
68/-- The negation-closed deviation-set property obtained from the functional
69equation does not force `0` to be the only realized deviation. -/
70theorem zeroDeviationSet_neg_closed_not_enough :
71 ∃ Ξ : CompletedXiSurface,
72 (1 / 2 : ℝ) ∈ zeroDeviationSet Ξ ∧
73 (-1 / 2 : ℝ) ∈ zeroDeviationSet Ξ ∧
74 0 ∉ zeroDeviationSet Ξ := by
75 refine ⟨toyCompletedXiSurface, ?_, ?_, ?_⟩
76 · refine ⟨(3 / 4 : ℂ), ?_, ?_⟩
77 · exact toyCompletedXiSurface_has_off_critical_zero.1
78 · norm_num [zeroDeviation]
79 · have hhalf : (1 / 2 : ℝ) ∈ zeroDeviationSet toyCompletedXiSurface := by
80 refine ⟨(3 / 4 : ℂ), ?_, ?_⟩
81 · exact toyCompletedXiSurface_has_off_critical_zero.1
82 · norm_num [zeroDeviation]
83 have hneg : (-(1 / 2 : ℝ)) ∈ zeroDeviationSet toyCompletedXiSurface :=
84 zeroDeviationSet_neg_closed toyCompletedXiSurface hhalf
85 norm_num at hneg ⊢
86 exact hneg
87 · intro hzero
88 rcases hzero with ⟨s, hs, hdev⟩
89 have hline : OnCriticalLine s :=
90 (zeroDeviation_eq_zero_iff_on_critical_line s).mp hdev
91 have hvalue :
92 toyCompletedXiSurface.xi s =
93 (((1 / 2 - 3 / 4) ^ 2 * (1 / 2 - 1 / 4) ^ 2 : ℝ) : ℂ) := by
94 simp [toyCompletedXiSurface, toyXi, show s.re = 1 / 2 by exact hline]
95 have hnonzero :
96 ((((1 / 2 - 3 / 4) ^ 2 * (1 / 2 - 1 / 4) ^ 2 : ℝ) : ℂ)) ≠ 0 := by
97 norm_num
98 have hxine : toyCompletedXiSurface.xi s ≠ 0 := by
99 simpa [hvalue] using hnonzero
100 exact hxine hs
101
102/-- The strongest concrete Vector C data currently available from pure
103completed-ξ symmetry plus the FE/RCL doubling law. -/
104structure PureVectorCDoublingData (Ξ : CompletedXiSurface) (ρ : ℂ) : Prop where
105 zero : Ξ.xi ρ = 0
106 reflection_zero : Ξ.xi (functionalReflection ρ) = 0
107 conjugation_zero : Ξ.xi (conj ρ) = 0
108 critical_reflection_zero : Ξ.xi (criticalReflection ρ) = 0
109 doubled_recurrence :
110 doubledZeroDefect ρ = 2 * (zeroDefect ρ) ^ 2 + 4 * zeroDefect ρ
111
112/-- Any actual completed-ξ zero carries the current pure Vector C package:
113pairing invariants plus the FE/RCL doubling recurrence. -/
114theorem pureVectorCDoublingData_of_zero (Ξ : CompletedXiSurface) {ρ : ℂ}
115 (hρ : Ξ.xi ρ = 0) :
116 PureVectorCDoublingData Ξ ρ := by
117 refine ⟨hρ, ?_, ?_, ?_, doubledZeroDefect_recurrence ρ⟩
118 · exact zero_pairing_under_reflection Ξ hρ
119 · exact zero_pairing_under_conjugation Ξ hρ
120 · exact zero_pairing_under_critical_reflection Ξ hρ
121
122/-- The current pure Vector C package is realized by an off-critical toy zero. -/
123theorem pureVectorCDoublingData_offline_example :
124 ∃ Ξ : CompletedXiSurface, ∃ ρ : ℂ,
125 PureVectorCDoublingData Ξ ρ ∧ ¬ OnCriticalLine ρ := by
126 refine ⟨toyCompletedXiSurface, (3 / 4 : ℂ), ?_, ?_⟩
127 · exact pureVectorCDoublingData_of_zero toyCompletedXiSurface
128 toyCompletedXiSurface_has_off_critical_zero.1
129 · exact toyCompletedXiSurface_has_off_critical_zero.2
130
131/-- Even after adding the current FE/RCL doubling law, pure completed-ξ
132symmetry data still cannot force a `ZeroCompositionWitness`.
133
134Therefore any successful upgrade from honest zeta-derived phase data to
135`ZeroCompositionWitness` must use genuinely extra analytic input not present in
136the pure FE package; in this repository the natural candidates live on the
137Euler/Hadamard side (`QuantitativeLocalFactorization`,
138`phaseIncrementEpsilonBound`, perturbation/budget control). -/
139theorem pureVectorCDoublingData_requires_extra_input :
140 ¬ (∀ (Ξ : CompletedXiSurface) (ρ : ℂ),
141 PureVectorCDoublingData Ξ ρ → Nonempty (ZeroCompositionWitness ρ)) := by
142 intro h
143 obtain ⟨Ξ, ρ, hpure, hline⟩ := pureVectorCDoublingData_offline_example
144 rcases h Ξ ρ hpure with ⟨w⟩
145 exact hline (zeroCompositionWitness_forces_on_critical_line w)
146
147/-- In particular, pure FE symmetry plus the current doubling law do not by
148themselves force the critical line. -/
149theorem pureVectorCDoublingData_not_enough_for_critical_line :
150 ¬ (∀ (Ξ : CompletedXiSurface) (ρ : ℂ),
151 PureVectorCDoublingData Ξ ρ → OnCriticalLine ρ) := by
152 intro h
153 obtain ⟨Ξ, ρ, hpure, hline⟩ := pureVectorCDoublingData_offline_example
154 exact hline (h Ξ ρ hpure)
155
156end
157
158end NumberTheory
159end IndisputableMonolith
160