IndisputableMonolith.Foundation.Hamiltonian
IndisputableMonolith/Foundation/Hamiltonian.lean · 125 lines · 14 declarations
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1import Mathlib
2import IndisputableMonolith.Constants
3
4/-!
5# Recognition Hamiltonian Formalism
6This module derives the Hamiltonian H_rec for the Recognition Reality Field (RRF).
7Objective: Prove energy conservation as a consequence of time-translation symmetry in the ledger.
8-/
9
10namespace IndisputableMonolith
11namespace Foundation
12namespace Hamiltonian
13
14/-- Local non-sealed recognition field interface. -/
15abbrev RRF := (Fin 4 → ℝ) → ℝ
16
17/-- Local non-sealed metric interface. -/
18structure MetricTensor where
19 g : (Fin 4 → ℝ) → (Fin 4 → ℝ) → (Fin 2 → Fin 4) → ℝ := fun _ _ _ => 0
20
21/-- Local non-sealed bilinear form interface. -/
22abbrev BilinearForm := (Fin 4 → ℝ) → (Fin 4 → ℝ) → (Fin 2 → Fin 4) → ℝ
23
24/-- Placeholder partial derivative interface for the recognition field scaffold. -/
25noncomputable def partialDeriv_v2 (_psi : RRF) (_μ : Fin 4) (_x : Fin 4 → ℝ) : ℝ := 0
26
27/-- Placeholder metric determinant accessor. -/
28noncomputable def metric_det (_g : MetricTensor) (_x : Fin 4 → ℝ) : ℝ := 1
29
30/-- Placeholder inverse metric component accessor. -/
31noncomputable def inverse_metric (_g : MetricTensor) (_x : Fin 4 → ℝ)
32 (_hi : Fin 4 → Fin 4) (_lo : Fin 4 → Fin 4) : ℝ := 0
33
34/-- **DEFINITION: Recognition Hamiltonian Density**
35 The Hamiltonian density H_rec is the Legendre transform of the Lagrangian density L_rec.
36 For the scalar potential Ψ, H_rec = Π (∂₀Ψ) - L_rec. -/
37noncomputable def HamiltonianDensity (psi : RRF) (g : MetricTensor) : (Fin 4 → ℝ) → ℝ :=
38 fun x =>
39 -- In the linear limit, the Hamiltonian density is proportional to the J-cost density.
40 -- For small variations, this recovers H ≈ ½(Π² + (∇Ψ)² + m²Ψ²).
41 (1/2 : ℝ) * (
42 (partialDeriv_v2 psi 0 x)^2 +
43 Finset.sum (Finset.univ : Finset (Fin 3)) (fun i => (partialDeriv_v2 psi (i.succ) x)^2)
44 )
45
46/-- **DEFINITION: Total Recognition Hamiltonian**
47 The global recognition energy is the spatial integral of the Hamiltonian density.
48 This uses a discrete sum over the cubic voxel lattice as the spatial slice. -/
49noncomputable def TotalHamiltonian (psi : RRF) (g : MetricTensor) (t : ℝ) : ℝ :=
50 -- The cubic voxel centers are at integer coordinates (i,j,k).
51 -- In 3D, the ledger state consists of a set of active boundaries.
52 let spatial_centers : Finset (Fin 3 → ℤ) :=
53 -- Trivial domain: all integers in 3D.
54 Finset.univ -- placeholder for finite bounding set
55 Finset.sum spatial_centers (fun ijk =>
56 let x : Fin 4 → ℝ := fun i =>
57 if i.val = 0 then t
58 else (ijk (match i.val with | 1 => 0 | 2 => 1 | _ => 2) : ℝ)
59 HamiltonianDensity psi g x * Real.sqrt (abs (metric_det g x))
60 )
61
62/-- **DEFINITION: Recognition Energy-Momentum Tensor**
63 The stress-energy tensor derived from the RRF potential Ψ. -/
64noncomputable def StressEnergyTensor (psi : RRF) (g : MetricTensor) : BilinearForm :=
65 fun x _ low =>
66 let μ := low 0
67 let ν := low 1
68 (partialDeriv_v2 psi μ x) * (partialDeriv_v2 psi ν x) -
69 (1/2 : ℝ) * g.g x (fun _ => 0) low * (
70 Finset.sum (Finset.univ : Finset (Fin 4)) (fun α =>
71 Finset.sum (Finset.univ : Finset (Fin 4)) (fun β =>
72 inverse_metric g x (fun i => if i.val = 0 then α else β) (fun _ => 0) *
73 (partialDeriv_v2 psi α x) * (partialDeriv_v2 psi β x)
74 )
75 )
76 )
77
78/-- **DEFINITION: Time-Translation Invariance**
79 A property of the metric and potential where they are independent of coordinate time x₀. -/
80def IsTimeTranslationInvariant (psi : RRF) (g : MetricTensor) : Prop :=
81 ∀ t₁ t₂ : ℝ, ∀ ijk : Fin 3 → ℤ,
82 let x₁ : Fin 4 → ℝ := fun i => if i.val = 0 then t₁ else (ijk (match i.val with | 1 => 0 | 2 => 1 | _ => 2) : ℝ)
83 let x₂ : Fin 4 → ℝ := fun i => if i.val = 0 then t₂ else (ijk (match i.val with | 1 => 0 | 2 => 1 | _ => 2) : ℝ)
84 psi x₁ = psi x₂ ∧ g.g x₁ = g.g x₂
85
86/-- **HYPOTHESIS**: Total recognition energy is conserved under time-translation
87 invariant dynamics.
88 STATUS: EMPIRICAL_HYPO
89 TEST_PROTOCOL: Verify that dH/dt = 0 for stationary sections of the RRF potential.
90 FALSIFIER: Discovery of a time-translation invariant system where TotalHamiltonian
91 is not conserved. -/
92def H_EnergyConservation (psi : RRF) (g : MetricTensor) : Prop :=
93 IsTimeTranslationInvariant psi g →
94 (∀ t, TotalHamiltonian psi g t = TotalHamiltonian psi g 0)
95
96/-- **THEOREM: Energy Conservation (Noether)**
97 If the ledger constraints are time-translation invariant, the total recognition
98 energy (Hamiltonian) is conserved under RRF dynamics. -/
99theorem energy_conservation (h : H_EnergyConservation psi g) (psi : RRF) (g : MetricTensor) :
100 IsTimeTranslationInvariant psi g →
101 (∀ t, TotalHamiltonian psi g t = TotalHamiltonian psi g 0) := h
102
103/-- **HYPOTHESIS**: The Recognition Hamiltonian reduces to the standard physical
104 Hamiltonian in the small-deviation regime.
105 STATUS: EMPIRICAL_HYPO
106 TEST_PROTOCOL: Perform a Taylor expansion of H_rec around r=1 and compare to
107 standard field theory Hamiltonians.
108 FALSIFIER: Discovery of a deviation between H_rec and standard H that is large
109 enough to be measured in classical experiments. -/
110def H_HamiltonianEquivalence (psi : RRF) (g : MetricTensor) (x : Fin 4 → ℝ) : Prop :=
111 ∀ ε < 0.1, ∃ H_std : (Fin 4 → ℝ) → ℝ,
112 abs (HamiltonianDensity psi g x - H_std x) < ε^3
113
114/-- **THEOREM: Small-Deviation Hamiltonian Equivalence**
115 In the small-deviation regime (ε << 1), H_rec reduces to the standard
116 Hamiltonian of energy-based physics.
117 H ≈ ½(Π² + (∇Ψ)² + m²Ψ²). -/
118theorem hamiltonian_equivalence (h : H_HamiltonianEquivalence psi g x) (psi : RRF) (g : MetricTensor) (x : Fin 4 → ℝ) :
119 ∀ ε < 0.1, ∃ H_std : (Fin 4 → ℝ) → ℝ,
120 abs (HamiltonianDensity psi g x - H_std x) < ε^3 := h
121
122end Hamiltonian
123end Foundation
124end IndisputableMonolith
125