IndisputableMonolith.QFT.CasimirRecognitionBoundary
IndisputableMonolith/QFT/CasimirRecognitionBoundary.lean · 148 lines · 16 declarations
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1import Mathlib
2import IndisputableMonolith.Cost
3import IndisputableMonolith.QFT.CasimirPlateModes
4
5/-!
6# Casimir Recognition Boundary
7
8Recognition Science reads the Casimir effect as a boundary-mode inventory
9imbalance. Conducting plates restrict admissible modes inside the gap; the
10renormalized cost-gradient of that restricted inventory is the pressure.
11
12This module proves the structural statements and keeps the electromagnetic
13boundary identification as a named bridge hypothesis.
14-/
15
16namespace IndisputableMonolith
17namespace QFT
18namespace CasimirRecognitionBoundary
19
20open Cost
21open CasimirPlateModes
22
23noncomputable section
24
25/-- A boundary-mode inventory compares the admissible interior mode weight with
26an exterior/reference mode weight. -/
27structure BoundaryModeInventory where
28 interior : ℝ
29 exterior : ℝ
30 interior_pos : 0 < interior
31 exterior_pos : 0 < exterior
32
33/-- The raw inventory deficit: exterior admissible weight minus interior
34admissible weight. Positive deficit is the parallel-plate Casimir case. -/
35noncomputable def modeInventoryDeficit (I : BoundaryModeInventory) : ℝ :=
36 I.exterior - I.interior
37
38/-- The positive exterior/interior ratio seen by the canonical reciprocal cost. -/
39noncomputable def inventoryRatio (I : BoundaryModeInventory) : ℝ :=
40 I.exterior / I.interior
41
42/-- Renormalized RS boundary cost for the inventory mismatch. -/
43noncomputable def renormalizedBoundaryCost (I : BoundaryModeInventory) : ℝ :=
44 Jcost (inventoryRatio I)
45
46/-- The inventory ratio is positive. -/
47theorem inventoryRatio_pos (I : BoundaryModeInventory) :
48 0 < inventoryRatio I := by
49 unfold inventoryRatio
50 exact div_pos I.exterior_pos I.interior_pos
51
52/-- Renormalized boundary cost is nonnegative. -/
53theorem renormalizedBoundaryCost_nonneg (I : BoundaryModeInventory) :
54 0 ≤ renormalizedBoundaryCost I := by
55 unfold renormalizedBoundaryCost
56 exact Jcost_nonneg (inventoryRatio_pos I)
57
58/-- Equal interior/exterior inventories have zero boundary cost. -/
59theorem renormalizedBoundaryCost_eq_zero_of_balanced
60 (I : BoundaryModeInventory) (h : I.exterior = I.interior) :
61 renormalizedBoundaryCost I = 0 := by
62 unfold renormalizedBoundaryCost inventoryRatio
63 rw [h, div_self (ne_of_gt I.interior_pos)]
64 exact Jcost_unit0
65
66/-- A positive inventory deficit is exactly `interior < exterior`. -/
67theorem deficit_pos_iff (I : BoundaryModeInventory) :
68 0 < modeInventoryDeficit I ↔ I.interior < I.exterior := by
69 unfold modeInventoryDeficit
70 constructor <;> intro h <;> linarith
71
72/-- If the exterior inventory is larger, the RS ratio exceeds one. -/
73theorem inventoryRatio_gt_one_of_deficit_pos
74 (I : BoundaryModeInventory) (h : 0 < modeInventoryDeficit I) :
75 1 < inventoryRatio I := by
76 have hlt : I.interior < I.exterior := (deficit_pos_iff I).mp h
77 unfold inventoryRatio
78 rw [one_lt_div I.interior_pos]
79 exact hlt
80
81/-- A nonzero positive deficit gives a strictly positive recognition cost. -/
82theorem renormalizedBoundaryCost_pos_of_deficit_pos
83 (I : BoundaryModeInventory) (h : 0 < modeInventoryDeficit I) :
84 0 < renormalizedBoundaryCost I := by
85 have hratio_pos := inventoryRatio_pos I
86 have hratio_gt : 1 < inventoryRatio I :=
87 inventoryRatio_gt_one_of_deficit_pos I h
88 unfold renormalizedBoundaryCost
89 exact Jcost_pos_of_ne_one (inventoryRatio I) hratio_pos (ne_of_gt hratio_gt)
90
91/-- A pressure gradient is a positive outward cost-gradient with pressure
92defined as minus that gradient. -/
93noncomputable def pressureFromCostGradient (gradient : ℝ) : ℝ :=
94 -gradient
95
96/-- Positive cost-gradient produces attractive pressure. -/
97theorem attractive_of_positive_cost_gradient
98 (gradient : ℝ) (hgradient : 0 < gradient) :
99 pressureFromCostGradient gradient < 0 := by
100 unfold pressureFromCostGradient
101 exact neg_neg_of_pos hgradient
102
103/-- Bridge hypothesis: electromagnetic conducting-boundary admissibility is
104represented by a boundary-mode inventory, and its regularized energy gradient
105matches the RS boundary-cost gradient. -/
106structure EMRecognitionBoundaryBridge where
107 inventory : PlateSeparation → BoundaryModeInventory
108 costGradient : PlateSeparation → ℝ
109 inducedPressure : PlateSeparation → ℝ
110 admissibility_matches_inventory : Prop
111 regularized_energy_matches_cost_gradient :
112 ∀ a : PlateSeparation, inducedPressure a = pressureFromCostGradient (costGradient a)
113
114/-- Under the bridge, a positive cost-gradient at a separation gives attractive
115pressure at that separation. -/
116theorem bridge_attractive_of_positive_gradient
117 (B : EMRecognitionBoundaryBridge) (a : PlateSeparation)
118 (hgradient : 0 < B.costGradient a) :
119 B.inducedPressure a < 0 := by
120 rw [B.regularized_energy_matches_cost_gradient a]
121 exact attractive_of_positive_cost_gradient (B.costGradient a) hgradient
122
123/-- Structural certificate for the RS boundary interpretation. -/
124structure RecognitionBoundaryCert where
125 cost_nonnegative :
126 ∀ I : BoundaryModeInventory, 0 ≤ renormalizedBoundaryCost I
127 balanced_zero :
128 ∀ I : BoundaryModeInventory,
129 I.exterior = I.interior → renormalizedBoundaryCost I = 0
130 deficit_positive_cost :
131 ∀ I : BoundaryModeInventory,
132 0 < modeInventoryDeficit I → 0 < renormalizedBoundaryCost I
133 positive_gradient_attractive :
134 ∀ gradient : ℝ, 0 < gradient → pressureFromCostGradient gradient < 0
135
136/-- Certificate for the theorem-level part of the boundary-mode reading. -/
137def recognitionBoundaryCert : RecognitionBoundaryCert where
138 cost_nonnegative := renormalizedBoundaryCost_nonneg
139 balanced_zero := renormalizedBoundaryCost_eq_zero_of_balanced
140 deficit_positive_cost := renormalizedBoundaryCost_pos_of_deficit_pos
141 positive_gradient_attractive := attractive_of_positive_cost_gradient
142
143end
144
145end CasimirRecognitionBoundary
146end QFT
147end IndisputableMonolith
148