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LeanPool.Superdiffusion.Support.HighContrast.Corridor.PhaseComparison.GridCoverage

GridCoverage #

Ported from scottnarmstrong/CoarseGraining at c7ddd76c08ade64fed1b8d2ca51be14dfee8deb4. Module imports, support namespace and local option directives adapted for Lean Pool.

Discrete uniform-grid corridor coverage count #

Phase comparison (Prop 4.4 of the high-moment paper, Armstrong–Kuusi–Loher, in preparation) is proved with the continuum σ-average replaced by a finite uniform grid gridPhase ℓ N j i = (j i) · ℓ / N for j : Fin d → Fin N. This file records the elementary grid-counting coverage bound that replaces the continuum corridor-coverage estimate e.corridor.coverage:

Only 4 ≤ ℓ and ℓ ≤ N are used; the constant 3 is not sharp (any C·N/ℓ is acceptable, absorbed into C_d downstream).

noncomputable def HCPolySupport.gridPhase {d : ℕ} (ℓ : ℝ) (N : ℕ) (j : Fin d → Fin N) :
Vec d

The finite uniform phase grid: gridPhase ℓ N j is the phase vector with i-th coordinate (j i)·ℓ/N.

Equations
Instances For
    @[simp]
    theorem HCPolySupport.gridPhase_apply {d : ℕ} (ℓ : ℝ) (N : ℕ) (j : Fin d → Fin N) (i : Fin d) :
    gridPhase ℓ N j i = ↑↑(j i) * ℓ / ↑N

    1-d heart #

    theorem HCPolySupport.card_gridHits_le {ℓ : ℝ} (hℓ : 4 ≤ ℓ) {N : ℕ} (hN : ℓ ≤ ↑N) (t : ℝ) :
    ↑{c : Fin N | ∃ (n : ℤ), |t - ↑↑c * ℓ / ↑N - ↑n * ℓ| < 1}.card ≤ 3 * ↑N / ℓ

    M0 (1-d count). For 4 ≤ ℓ and ℓ ≤ N, at most 3N/ℓ of the grid points c ↦ c·ℓ/N, c : Fin N, lie within sup-distance 1 of t modulo the lattice ℓ·ℤ.

    d-dim corollary #

    theorem HCPolySupport.sum_indicator_gridPhase_corridor_le {d : ℕ} [NeZero d] {ℓ : ℝ} (hℓ : 4 ≤ ℓ) {N : ℕ} (hN : ℓ ≤ ↑N) (x : Vec d) :
    ∑ j : Fin d → Fin N, (corridorSet ℓ (gridPhase ℓ N j)).indicator (fun (x : Vec d) => 1) x ≤ 3 * ↑d / ℓ * ↑N ^ d

    M0 (d-dim coverage). For a fixed x and 4 ≤ ℓ ≤ N, the sum over the finite grid j : Fin d → Fin N of the corridor indicators of the phases gridPhase ℓ N j at x is at most (3d/ℓ)·N^d. Dividing by N^d, the grid average of 𝟙_{corridorSet} at any point is at most 3d/ℓ.