Canonical attraction #
The Gaussian Abelian argument reuses the square-weighted absolute-step measure
and the Taylor/Fubini identities from LaplaceExpansion. At Karamata index zero,
its transform is asymptotic to the truncated second moment. Two integrations
supply the factor 1/2; unboundedness makes the atom and centering corrections
negligible. The one-step expansions then imply attraction through Laplace continuity.
For finite positive variance, a general characteristic-function CLT supplies the
Gaussian limit directly, without a lower support assumption.
Ported from BGWLeaves/StableAnalysis/CanonicalAttraction.lean of the author's arXiv:1110.2163v4
formalization (local snapshot of 6 November 2026).
At the Gaussian boundary the damped second moment is asymptotic to K.
The absolute-step exponential remainder on the Gaussian scale.
Every fixed deterministic quadratic error is negligible when K → ∞.
The uncentered Gaussian Laplace remainder.
Gaussian D1: the centered remainder is asymptotic to K(x)/(2 x²).
Gaussian D1 in asymptotic-equivalence form at zero from the right.
The Gaussian canonical norming diverges.
Slow variation and the exact Gaussian crossing identify the scaled moment.
Gaussian D1: the one-step limit on the canonical norming.
A one-step centered Laplace expansion gives attraction after taking powers. The centering factor here is exactly the one used by the continuity provider.
D2(i): regularly varying right tail, with index strictly between one and two.
D2(ii): the infinite-variance Gaussian criterion.
D2(iii) in the critical offspring-law setting already covered by BGW.
D2(iii) for a general integer law of finite, strictly positive variance. No lower support bound is needed for this CLT proof. Positive variance excludes the degenerate case, whose canonical norming is identically zero.