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).
If the symmetrized law has a finite second moment, H(s)/s tends to it.
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.
The smoothing is bounded above by its linear finite-moment majorant.
Attraction excludes a degenerate symmetrized second moment.
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.
D3 in the positive, reciprocal-coordinate predicate expected by B1.
Dividing the smoothing by its parameter gives the Laplace exponent needed for the integrated squared-difference tail, including the boundary exponent zero.
Tail of the squared independent difference.
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Locally finite measure whose density is the squared-difference tail.
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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.
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.
The truncated moment is dominated by the capped moment.
Infinite second moment forces the capped moments to diverge.
Desymmetrization transfers the integrated-tail variation to the original capped moment.
Monotone density for the original capped moments.
Below index two, monotone density identifies the tail of the original square.
D4, non-Gaussian branch: attraction with infinite second moment forces
regular variation of the right tail with index -θ.
Capped and truncated moments differ by the endpoint tail term.
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.