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BGW.StableTrees.Attraction.DomainCriterion

Consequences of the Gaussian-smoothed converse #

For infinite second moment, Fubini identifies H(s)/s as the Laplace transform of the squared-difference tail density. Karamata and monotone density recover regular variation of its integrated tail. A uniform capped-moment comparison transfers this to the original step; a second application of monotone density recovers its squared tail, or the truncated moment at the Gaussian boundary.

The finite second moment case is obtained directly by dominated convergence, without a Tauberian theorem or a calculation of the smoothing constant.

Main exports: rightTail_regularlyVarying, truncSecondMoment_slowlyVarying_unbounded, index_eq_two_of_integrable_sq, and smoothing_isEquivalent_variance. Ported from BGWLeaves/StableAnalysis/DomainCriterion.lean of the author's arXiv:1110.2163v4 formalization (local snapshot of 6 November 2026).

theorem BGW.StableTrees.Attraction.DomainCriterion.smoothing_quotient_bounds {s x : ℝ} (hs : 0 < s) :
0 ≤ (1 - Real.exp (-s * x ^ 2)) / s ∧ (1 - Real.exp (-s * x ^ 2)) / s ≤ x ^ 2

The elementary bound used to dominate the smoothing difference quotient.

Finite second moment is preserved by independent symmetrization.

The independent difference has second moment twice the original variance.

The finite-variance expansion, in a form that also includes the degenerate law.

A finite-variance law attracted to a stable law has positive variance.

Finite second moment forces the Gaussian stable index. No support assumption is needed for this direction.

In the attracting finite-variance case the linear smoothing asymptotic is nonzero, hence it can also be stated as asymptotic equivalence.

Every positive smoothing parameter has strictly positive defect under attraction.

Dividing the smoothing by its parameter gives the Laplace exponent needed for the integrated squared-difference tail, including the boundary exponent zero.

The layer-cake/Fubini identity that turns D3 into the transform hypothesis of B1.

The cumulative mass of the tail-density measure is the integrated tail.

The Tauberian output for the symmetrized squared step, valid also at index two.

The monotone density conclusion, including its zero limit at the Gaussian boundary.

Below the Gaussian index, the squared-difference tail itself is regularly varying.

theorem BGW.StableTrees.Attraction.DomainCriterion.capped_difference_bound (a b x : ℝ) :
|min ((a - b) ^ 2) (x ^ 2) - min (a ^ 2) (x ^ 2) - min (b ^ 2) (x ^ 2)| ≤ 2 * |a * b|

Uniform pointwise comparison of capped squared differences and capped squares.

theorem BGW.StableTrees.Attraction.DomainCriterion.integral_min_sq_eq_integrated_tail {Ω : Type u_1} [MeasurableSpace Ω] (μ : MeasureTheory.Measure Ω) [MeasureTheory.IsProbabilityMeasure μ] (X : Ω → ℝ) (hX : Measurable X) {y : ℝ} (hy : 0 ≤ y) :
∫ (ω : Ω), min (X ω ^ 2) y ∂μ = ∫ (t : ℝ) in 0..y, μ.real {ω : Ω | t < X ω ^ 2}

Layer cake for a capped square. This form needs no second-moment hypothesis.

Capped second moment, with the cutoff in squared coordinates.

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    The bounded-error desymmetrization estimate.

    Desymmetrization transfers the integrated-tail variation to the original capped moment.

    Tail of the square of the original step.

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      Monotone density for the original capped moments.

      Below index two, monotone density identifies the tail of the original square.

      Bounded negative support removes the negative contribution to the squared tail.

      theorem BGW.StableTrees.Attraction.DomainCriterion.rightTail_regularlyVarying {ν : MeasureTheory.Measure ℤ} [MeasureTheory.IsProbabilityMeasure ν] {θ : ℝ} {b : ℕ → ℝ} (hb : IsStableAttracted ν θ (mean ν) b) (hneg : ν {z : ℤ | z < -1} = 0) (hint : MeasureTheory.Integrable (fun (z : ℤ) => ↑z) ν) (hinf : ¬MeasureTheory.Integrable (fun (z : ℤ) => ↑z ^ 2) ν) (hθ : θ < 2) :
      MonotoneDensity.IsRegVaryAtTop (fun (x : ℝ) => ν.real {z : ℤ | x < ↑z}) (-θ)

      D4, non-Gaussian branch: attraction with infinite second moment forces regular variation of the right tail with index -θ.

      D4, Gaussian branch: infinite second moment and Gaussian attraction imply slow variation and divergence of the truncated second moment. The proof needs no support bound, because the capped-moment comparison already handles both tails.

      Stable attraction below index two automatically has infinite second moment.