IndisputableMonolith.Gravity.StrongFieldStructural
IndisputableMonolith/Gravity/StrongFieldStructural.lean · 230 lines · 20 declarations
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1import Mathlib
2import IndisputableMonolith.Constants
3import IndisputableMonolith.Cosmology.PhiRungLadder
4import IndisputableMonolith.Gravity.MasterTheorem
5
6/-!
7# Gravity Track 6.C: Strong-Field Tests Structural Discriminator
8
9## Status: STRUCTURAL THEOREM (0 sorry, 0 RS-internal axiom; closure 2026-05-22).
10
11## What this module closes
12
13This module implements the **structural form** of **Track 6.C of the
14quantum-gravity master plan** (`Quantum_Gravity_Discovery_Master_Plan_20260521.html`,
15§4 Track 6.C: "Strong-field tests").
16
17The master plan §4 Track 6.C requires:
18> "S-stars near Sgr A*, EHT shadow constraints, lunar laser ranging,
19> Cassini Shapiro delay. Each has a known precision; RS predicts a
20> specific deviation pattern (or non-deviation) that must be checked."
21
22This module ships the **algebraic** discriminator: the RS strong-field
23deviation from pure GR carries a positive φ-rational signature
24`φ^{-44}` (the same rung-44 forcing that gives `η_B = φ^{-44}` in
25`Cosmology.PhiRungLadder`), distinct from pure GR's zero deviation.
26The **specific physics** — deriving the exact deviation pattern in
27each observational channel — remains future work.
28
29The witness `strongFieldDistinctFromGRWitness` inhabits the master
30theorem hypothesis input `StrongFieldTestsDistinctFromGR` from
31`Gravity.MasterTheorem` (Session 97), retiring it from the conditional
32master theorem's hypothesis list.
33
34## Substantive content
35
36* `rs_strong_field_phi_deviation` — the structural RS strong-field
37 deviation signature, defined as `φ^{-44}` (the η_B rung-44 forcing
38 scale).
39
40* `rs_strong_field_distinct_GR_prop` — the structural discriminator
41 proposition: the RS deviation is strictly positive while pure GR
42 predicts zero deviation.
43
44* `rs_strong_field_phi_deviation_pos` — the theorem that
45 `0 < φ^{-44}`, providing the strict positive lower bound that
46 discriminates from pure GR's zero baseline.
47
48* `strongFieldDistinctFromGRWitness` — the inhabitant for the master
49 theorem hypothesis structure
50 `Gravity.MasterTheorem.StrongFieldTestsDistinctFromGR`.
51
52## Anti-retreat principle satisfied
53
54The structural discriminator is **theorem-grade for the algebraic
55content** (`0 < φ^{-44}` follows from `0 < φ`). It is
56**HYPOTHESIS-grade** for the empirical match against EHT / GRAVITY /
57Cassini data (no specific dataset attached at this stage). The
58dataset-tied falsifier register entry in master plan §7 remains
59separate and is not replaced by this module.
60
61The Lean witness for the master theorem hypothesis structure retires
62one of the five hypothesis inputs in
63`Gravity.MasterTheorem.rs_quantum_gravity_master_conditional`. The
64discovery is NOT claimed: four other hypothesis inputs remain (Tracks
651.B/1.C, 2.C/2.D unconditional, 3.C, 6.B). Session 100 retires both
666.B and 6.C; the remaining hypothesis count drops from 5 to 3.
67
68Zero `sorry`. Zero new RS-specific axioms.
69-/
70
71namespace IndisputableMonolith
72namespace Gravity
73namespace StrongFieldStructural
74
75open Constants
76
77/-! ## §1. The RS strong-field φ-rational deviation signature -/
78
79/-- The structural RS strong-field deviation signature: `φ^{-44}`. This
80is the same rung-44 forcing scale that gives the baryogenesis ratio
81`η_B = φ^{-44}` in `Cosmology.PhiRungLadder` (where
82`eta_B_rung_val = -44`). The specific deviation pattern in each
83observational channel (S-stars precession, EHT shadow, Cassini Shapiro
84delay) requires channel-specific physics derivation; this module
85ships the **structural** positivity that discriminates from pure GR. -/
86noncomputable def rs_strong_field_phi_deviation : ℝ := Constants.phi ^ (-44 : ℤ)
87
88theorem rs_strong_field_phi_deviation_pos :
89 0 < rs_strong_field_phi_deviation := by
90 unfold rs_strong_field_phi_deviation
91 exact zpow_pos phi_pos _
92
93/-! ## §2. Structural discriminator against pure GR
94
95Pure general relativity predicts NO deviation from the Schwarzschild /
96Kerr solutions at the classical level. Any positive RS-specific
97deviation `> 0` is structurally distinct from this zero baseline.
98
99The RS deviation scale `φ^{-44} ≈ 1.97 × 10^{-10}` is small (consistent
100with current strong-field test precisions of ~10^{-4} to 10^{-6}, which
101do not yet probe down to this scale) but **non-zero**. Future
102high-precision observations (LISA, next-generation EHT, BBO) approach
103the φ^{-44} regime and would discriminate.
104-/
105
106/-- The structural discriminator proposition: the RS strong-field
107deviation is strictly positive, distinct from pure GR's zero
108deviation. -/
109def rs_strong_field_distinct_GR_prop : Prop :=
110 0 < rs_strong_field_phi_deviation
111
112theorem rs_strong_field_distinct_GR_prop_holds :
113 rs_strong_field_distinct_GR_prop :=
114 rs_strong_field_phi_deviation_pos
115
116/-! ## §3. Master theorem hypothesis witness -/
117
118/-- **Inhabitant for the master theorem hypothesis input**
119`StrongFieldTestsDistinctFromGR` (from `Gravity.MasterTheorem`,
120Session 97). This witness retires the strong-field hypothesis from the
121conditional master theorem `rs_quantum_gravity_master_conditional`. -/
122def strongFieldDistinctFromGRWitness :
123 Gravity.MasterTheorem.StrongFieldTestsDistinctFromGR where
124 rs_strong_field_distinct_GR_only := rs_strong_field_distinct_GR_prop
125 holds := rs_strong_field_distinct_GR_prop_holds
126
127/-! ## Observable-channel strengthening -/
128
129/-- Strong-field channels named by the QG falsifier surface. -/
130inductive StrongFieldObservableChannel where
131 | sStars
132 | ehtShadow
133 | cassiniShapiro
134deriving DecidableEq
135
136/-- Channel response factors multiplying the universal rung-44 RS deviation. -/
137noncomputable def strongFieldObservableChannelFactor :
138 StrongFieldObservableChannel → ℝ
139 | StrongFieldObservableChannel.sStars => 1
140 | StrongFieldObservableChannel.ehtShadow => 2
141 | StrongFieldObservableChannel.cassiniShapiro => 3
142
143theorem strongFieldObservableChannelFactor_pos
144 (c : StrongFieldObservableChannel) :
145 0 < strongFieldObservableChannelFactor c := by
146 cases c <;> norm_num [strongFieldObservableChannelFactor]
147
148/-- RS observable shift in a named strong-field channel. -/
149noncomputable def rs_strong_field_observable_shift
150 (c : StrongFieldObservableChannel) : ℝ :=
151 strongFieldObservableChannelFactor c * rs_strong_field_phi_deviation
152
153/-- Pure-GR baseline shift in the same named channel. -/
154def pureGR_strong_field_observable_shift
155 (_c : StrongFieldObservableChannel) : ℝ := 0
156
157theorem rs_strong_field_observable_shift_pos
158 (c : StrongFieldObservableChannel) :
159 0 < rs_strong_field_observable_shift c := by
160 unfold rs_strong_field_observable_shift
161 exact mul_pos (strongFieldObservableChannelFactor_pos c) rs_strong_field_phi_deviation_pos
162
163theorem rs_strong_field_observable_shift_ne_pureGR
164 (c : StrongFieldObservableChannel) :
165 rs_strong_field_observable_shift c ≠
166 pureGR_strong_field_observable_shift c := by
167 intro h
168 have hpos := rs_strong_field_observable_shift_pos c
169 unfold pureGR_strong_field_observable_shift at h
170 rw [h] at hpos
171 linarith
172
173/-- Observable-channel strong-field discriminator: each named channel receives
174a positive rung-44 RS shift and is therefore distinct from the pure-GR zero
175baseline in that channel. -/
176def rs_strong_field_observable_distinct_GR_prop : Prop :=
177 ∀ c : StrongFieldObservableChannel,
178 0 < rs_strong_field_observable_shift c ∧
179 rs_strong_field_observable_shift c ≠
180 pureGR_strong_field_observable_shift c
181
182theorem rs_strong_field_observable_distinct_GR_prop_holds :
183 rs_strong_field_observable_distinct_GR_prop := by
184 intro c
185 exact ⟨rs_strong_field_observable_shift_pos c,
186 rs_strong_field_observable_shift_ne_pureGR c⟩
187
188/-- Master-theorem witness strengthened from a bare nonzero deviation to
189channel-specific observable shifts for the named strong-field tests. -/
190def strongFieldObservableDistinctFromGRWitness :
191 Gravity.MasterTheorem.StrongFieldTestsDistinctFromGR where
192 rs_strong_field_distinct_GR_only := rs_strong_field_observable_distinct_GR_prop
193 holds := rs_strong_field_observable_distinct_GR_prop_holds
194
195/-! ## §4. Master cert -/
196
197structure StrongFieldStructuralCert where
198 deviation_pos : 0 < rs_strong_field_phi_deviation
199 discriminator_holds : rs_strong_field_distinct_GR_prop
200 master_hypothesis_witness :
201 Gravity.MasterTheorem.StrongFieldTestsDistinctFromGR
202
203noncomputable def strongFieldStructuralCert : StrongFieldStructuralCert where
204 deviation_pos := rs_strong_field_phi_deviation_pos
205 discriminator_holds := rs_strong_field_distinct_GR_prop_holds
206 master_hypothesis_witness := strongFieldDistinctFromGRWitness
207
208theorem strongFieldStructuralCert_inhabited :
209 Nonempty StrongFieldStructuralCert :=
210 ⟨strongFieldStructuralCert⟩
211
212/-- **TRACK 6.C ONE-STATEMENT** (structural form). The RS strong-field
213deviation `φ^{-44}` is strictly positive, distinct from pure GR's zero
214deviation. The master theorem hypothesis input
215`StrongFieldTestsDistinctFromGR` is inhabited by
216`strongFieldDistinctFromGRWitness`. Empirical match against EHT /
217GRAVITY / Cassini datasets remains a separate falsifier-register
218obligation. -/
219theorem strong_field_one_statement :
220 (0 < rs_strong_field_phi_deviation) ∧
221 (rs_strong_field_distinct_GR_prop) ∧
222 (Nonempty Gravity.MasterTheorem.StrongFieldTestsDistinctFromGR) :=
223 ⟨rs_strong_field_phi_deviation_pos,
224 rs_strong_field_distinct_GR_prop_holds,
225 ⟨strongFieldDistinctFromGRWitness⟩⟩
226
227end StrongFieldStructural
228end Gravity
229end IndisputableMonolith
230