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PhaseFringeDensity
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IndisputableMonolith.Relativity.Lensing.ShadowPredictions on GitHub at line 21.
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18/-- **DEFINITION: Phase Fringe Density**
19 The density of the interference fringe at the event horizon boundary.
20 $\rho_{fringe} = \sin(2\pi \cdot t / (8\tau_0))$ where t is the local tick coordinate. -/
21noncomputable def PhaseFringeDensity (tau0 : ℝ) (t : ℝ) : ℝ :=
22 Real.sin (2 * Real.pi * t / (8 * tau0))
23
24/-- **DEFINITION: ILG Lensing Correction**
25 The modification to the deflection angle $\delta \theta$ due to the 8-tick cycle.
26 $\delta \theta_{ILG} = \delta \theta_{GR} \cdot (1 + \epsilon_{fringe})$. -/
27noncomputable def LensingCorrection (delta_theta_gr : ℝ) (epsilon_fringe : ℝ) : ℝ :=
28 delta_theta_gr * (1 + epsilon_fringe)
29
30/-- **THEOREM: Shadow Fringe Existence**
31 The 8-tick cycle forces a non-zero phase fringe at the event horizon
32 of any Schwarzschild-like black hole in the RS framework. -/
33theorem shadow_fringe_exists (tau0 : ℝ) (h_tau0 : tau0 > 0) :
34 ∃ (rho : ℝ → ℝ), ∀ t, rho t = PhaseFringeDensity tau0 t ∧ (∃ t', rho t' ≠ 0) := by
35 use PhaseFringeDensity tau0
36 intro t
37 constructor
38 · rfl
39 · use 2 * tau0
40 unfold PhaseFringeDensity
41 -- sin(2π * 2τ0 / (8τ0)) = sin(π/2) = 1
42 have h : 2 * Real.pi * (2 * tau0) / (8 * tau0) = Real.pi / 2 := by
43 field_simp [h_tau0]
44 ring
45 rw [h]
46 simp [Real.sin_pi_div_two]
47
48/-- **CERT(definitional): Shadow Diameter Correction**
49 The predicted diameter of the black hole shadow is shifted by the ILG
50 fringe factor $\epsilon_{fringe} \sim \lambda_{rec} / R_s$.
51