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BGW.StableTrees.Attraction.GaussianSmoothing

Gaussian smoothing of an attracted step law #

The characteristic-function defect is obtained at moving frequencies. The centering phase disappears on taking moduli. The exponent of the squared stable modulus is 2 * cos (π * θ / 2) * |t| ^ θ, which is negative for nonzero t. Ported from BGWLeaves/StableAnalysis/GaussianSmoothing.lean of the author's arXiv:1110.2163v4 formalization (local snapshot of 6 November 2026).

The squared stable modulus, with its (negative) exponent explicit.

theorem BGW.StableTrees.Attraction.GaussianSmoothing.tendsto_nat_mul_one_sub_of_pow {x : ℕ → ℝ} {k : ℕ → ℕ} {L : ℝ} (hx : Filter.Tendsto x Filter.atTop (nhds 1)) (hp : Filter.Tendsto (fun (n : ℕ) => x n ^ k n) Filter.atTop (nhds (Real.exp L))) :
Filter.Tendsto (fun (n : ℕ) => ↑(k n) * (1 - x n)) Filter.atTop (nhds (-L))

A power limit gives the first-order defect once the bases tend to one. The derivative is extended at one, so the bases are allowed to equal one.

Attraction controls the squared one-step CF powers at moving frequencies.

The symmetrized characteristic-function defect, including moving frequencies. No step lower bound or first-moment hypothesis is needed for this implication.

The fixed-frequency specialization used in Gaussian smoothing.

The defect limit also holds along arbitrary diverging time changes.

theorem BGW.StableTrees.Attraction.GaussianSmoothing.eventually_stepCharFun_defect_le_on_Icc {ν : MeasureTheory.Measure ℤ} [MeasureTheory.IsProbabilityMeasure ν] {θ m : ℝ} {b : ℕ → ℝ} (hb : IsStableAttracted ν θ m b) (R : ℝ) :
∃ (C : ℝ), 0 < C ∧ ∃ (N : ℕ), ∀ n ≥ N, ∀ t ∈ Set.Icc (-R) R, ↑n * (1 - ‖TransformConvergence.stepCharFun ν (t / b n)‖ ^ 2) ≤ C

Compact-frequency boundedness, obtained from the moving-frequency defect limit.

The law of the difference of two independent copies of the step.

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  • One or more equations did not get rendered due to their size.
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    Product-law realization of the independent difference.

    The smoothing integrand is bounded and integrable for every nonnegative parameter.

    The smoothing takes values in the unit interval.

    Smoothing is monotone, the property needed to interpolate between adjacent scales.

    Elementary telescoping bound on powers in the closed complex unit disk.

    theorem BGW.StableTrees.Attraction.GaussianSmoothing.one_sub_re_pow_le {z : ℂ} (hz : ‖z‖ = 1) (k : ℕ) :
    1 - (z ^ k).re ≤ ↑k ^ 2 * (1 - z.re)

    The pointwise quadratic integer-multiple bound behind CF domination.

    Quadratic control of the real CF defect at integer multiples.

    theorem BGW.StableTrees.Attraction.GaussianSmoothing.eventually_stepCharFun_defect_le_quadratic {ν : MeasureTheory.Measure ℤ} [MeasureTheory.IsProbabilityMeasure ν] {θ m : ℝ} {b : ℕ → ℝ} (hb : IsStableAttracted ν θ m b) :
    ∃ (C : ℝ), 0 < C ∧ ∃ (N : ℕ), ∀ n ≥ N, ∀ (t : ℝ), ↑n * (1 - ‖TransformConvergence.stepCharFun ν (t / b n)‖ ^ 2) ≤ C * (1 + t ^ 2)

    A global quadratic bound, uniform in the walk length after a fixed threshold.

    Integrating the scaled CF defects gives the Gaussian integral limit.

    The positive finite smoothing constant; no Gamma evaluation is needed.

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      Strict positivity of the Gaussian moment gives strict positivity of the constant.

      The Gaussian integral limit with its homogeneous constant factored out.

      The scale form consumed by the domain-of-attraction converse.

      Gaussian smoothing limits remain valid under moving scales and time changes.

      A sequence with asymptotically unit adjacent ratios has asymptotically exact first crossings, even if it is not monotone.

      Continuum scale ratios, first stated at infinity in the inverse scale variable.

      Gaussian-smoothed converse: the smoothed symmetrized squared-step defect is regularly varying at zero from the right, with index θ / 2. This conclusion holds for arbitrary eventually positive attracting normings.