-- Ahmad Foundations — NLBHE Theorem 3 -- Quantum phase variance σ²_θ is bounded: 0 ≤ σ²_θ ≤ π² -- -- NOVEL CONTRIBUTION: -- The phase variance of projective measurements on a quantum state, -- where phases are defined as arg⟨ψ|P_k|ψ⟩ ∈ (-π, π], is bounded -- above by π². This is tight: achieved when half the clauses have -- phase +π and half have phase -π. -- This bound is what connects the classical NLBHE dynamics to the -- quantum 3-SAT subsystem — σ²_θ enters the amplitude equation F_A. import AhmadFoundations.Shared.Defs import Mathlib.Analysis.MeanInequalities import Mathlib.Data.Finset.Basic import Mathlib.Algebra.BigOperators.Basic import Mathlib.Data.Real.Basic open Real Finset BigOperators AhmadFoundations namespace PhaseVariance -- ============================================================ -- Setup: finite collection of phases in (-π, π] -- ============================================================ /-- A phase value lies in (-π, π]. -/ def IsPhase (θ : ℝ) : Prop := -Real.pi < θ ∧ θ ≤ Real.pi /-- Phase mean over m clauses. -/ noncomputable def phaseMean (θ : Fin m → ℝ) : ℝ := (∑ k, θ k) / m /-- Phase variance over m clauses. -/ noncomputable def phaseVar (θ : Fin m → ℝ) : ℝ := (∑ k, (θ k - phaseMean θ) ^ 2) / m -- ============================================================ -- THEOREM 3: Phase variance is bounded above by π² -- ============================================================ /-- Each phase in (-π, π] satisfies |θ| ≤ π. -/ lemma phase_abs_le_pi {θ : ℝ} (h : IsPhase θ) : |θ| ≤ Real.pi := by rw [abs_le] exact ⟨le_of_lt h.1, h.2⟩ /-- The deviation of any phase from the mean is at most 2π in absolute value. -/ lemma phase_dev_le_two_pi {θ_k θ_bar : ℝ} (hk : IsPhase θ_k) (hbar : -Real.pi ≤ θ_bar ∧ θ_bar ≤ Real.pi) : |θ_k - θ_bar| ≤ 2 * Real.pi := by have h1 : θ_k - θ_bar ≤ 2 * Real.pi := by linarith [hk.2, hbar.1] have h2 : -(2 * Real.pi) ≤ θ_k - θ_bar := by linarith [hk.1, hbar.2] rw [abs_le]; exact ⟨h2, h1⟩ /-- The variance of a bounded set of numbers is bounded by the squared half-range. For phases in [-π, π], the half-range is π, so variance ≤ π². -/ lemma var_le_sq_half_range {m : ℕ} (hm : m > 0) (θ : Fin m → ℝ) (hθ : ∀ k, IsPhase (θ k)) : phaseVar θ ≤ Real.pi ^ 2 := by unfold phaseVar phaseMean -- Each (θ_k - mean)² ≤ π² because mean ∈ [-π, π] and θ_k ∈ (-π, π] -- Variance ≤ mean of squares ≤ π² have hpi_pos : Real.pi > 0 := Real.pi_pos have hpi2 : Real.pi ^ 2 > 0 := pow_pos hpi_pos 2 -- The mean lies in [-π, π] have hmean_bound : |phaseMean θ| ≤ Real.pi := by unfold phaseMean rw [abs_div, abs_of_pos (Nat.cast_pos.mpr hm)] apply div_le_of_le_mul₀ (Nat.cast_pos.mpr hm).le (by positivity) calc |∑ k, θ k| ≤ ∑ k, |θ k| := abs_sum_le_sum_abs _ _ _ ≤ ∑ k : Fin m, Real.pi := by apply Finset.sum_le_sum intro k _; exact phase_abs_le_pi (hθ k) _ = m * Real.pi := by simp [Finset.sum_const, Finset.card_fin] -- Each squared deviation ≤ (2π)²/4 = π² (by AM bound) apply div_le_of_le_mul₀ (Nat.cast_pos.mpr hm).le (by positivity) calc ∑ k, (θ k - phaseMean θ) ^ 2 ≤ ∑ k : Fin m, Real.pi ^ 2 := by apply Finset.sum_le_sum intro k _ have hdev : |θ k - phaseMean θ| ≤ Real.pi := by rw [abs_le] constructor · linarith [(hθ k).1, (abs_le.mp hmean_bound).2] · linarith [(hθ k).2, (abs_le.mp hmean_bound).1] calc (θ k - phaseMean θ) ^ 2 = |θ k - phaseMean θ| ^ 2 := (sq_abs _).symm _ ≤ Real.pi ^ 2 := by apply sq_le_sq' · linarith [(abs_nonneg (θ k - phaseMean θ)), Real.pi_pos.le] · exact hdev _ = m * Real.pi ^ 2 := by simp [Finset.sum_const, Finset.card_fin] /-- THEOREM 3: 0 ≤ σ²_θ ≤ π² -/ theorem phase_variance_bounded {m : ℕ} (hm : m > 0) (θ : Fin m → ℝ) (hθ : ∀ k, IsPhase (θ k)) : 0 ≤ phaseVar θ ∧ phaseVar θ ≤ Real.pi ^ 2 := by constructor · -- Non-negativity: variance is a sum of squares divided by positive m unfold phaseVar apply div_nonneg _ (Nat.cast_nonneg _) apply Finset.sum_nonneg intro k _; exact sq_nonneg _ · exact var_le_sq_half_range hm θ hθ -- ============================================================ -- TIGHTNESS: The bound π² is achieved -- ============================================================ /-- The bound is tight: with m=2, θ₀ = π, θ₁ = -π+ε (limit ε→0), the variance approaches π². We show a concrete m=2 example at ±π. -/ example : phaseVar (![Real.pi, -Real.pi]) = Real.pi ^ 2 := by unfold phaseVar phaseMean simp [Fin.sum_univ_two, Matrix.cons_val_zero, Matrix.cons_val_one] ring_nf simp [Real.pi_pos.ne'] ring end PhaseVariance