LatticeCount #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The triadic lattice annulus is finite, with an explicit count #
ABK26, §4.1, l.good.scales.ratio.lambda, the per-annulus atom tail: the
union-bound penalty C(n−k+1)³ of the lattice maximum
max_{z ∈ 3^{k−2}ℤ^d ∩ (□_n ∖ □_{n−1})} ( … )_+
This module proves it.
What is proved #
abs_le_of_mem_latticeCubeSet— a lattice point of spacing3^jinside□_outerhas integer coordinates bounded by3^{outer−j}(crude by a factor2, which costs nothing downstream).latticeAnnulusFinset— theFinsetof those index vectors, withcard_latticeAnnulusFinset_legiving# ≤ 3^{d(outer−j+1)}.log_card_latticeAnnulusFinset_le— the form the union bound consumes, andannulusPenalty/log_card_le_annulusPenalty_rpow_sub_one— the admissible penaltycofisBigOWith_fmax, which atσ = 1/3is a cubic inouter − j, the manuscript'sC(n−k+1)³.
Scope #
Provider material: proved local helpers. Pure geometry and counting; no probability, no model, no standing assumption.
References #
- ABK26,
l.good.scales.ratio.lambda.
1. The coordinate bound #
A triadic lattice point of spacing 3^j inside □_outer has bounded
index. The sharp bound is (3^{outer−j} − 1)/2; the crude 3^{outer−j} used
here avoids an integer division and costs only a bounded factor in the
logarithm.
2. The enclosing box and its cardinality #
The Finset of integer index vectors with all coordinates in [-B, B].
Equations
- Algsuperdiff.Section4.Provider.Proportion.boxIndexFinset d B = Fintype.piFinset fun (x : Fin d) => Finset.Icc (-B) B
Instances For
The lattice annulus as a Finset. The proved set
Support.latticeAnnulusSet cut out of the enclosing index box.
Equations
- One or more equations did not get rendered due to their size.
Instances For
4. The union-bound penalty #
The annular counting penalty in the proportion tail estimate.
Equations
Instances For
The defining property of the penalty: it clears the isBigOWith_fmax
interface log(#S) ≤ c^σ − 1 at the lattice annulus.