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).
Removing the deterministic centering phase from the squared modulus.
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.
Compact-frequency boundedness, obtained from the moving-frequency defect limit.
The law of the difference of two independent copies of the step.
Equations
- One or more equations did not get rendered due to their size.
Instances For
The symmetrized CF is the squared modulus of the original CF.
Product-law realization of the independent difference.
Gaussian-smoothed squared-step defect.
Equations
Instances For
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.
Quadratic control of the real CF defect at integer multiples.
Integer-multiple control specialized to the symmetrized step law.
A global quadratic bound, uniform in the walk length after a fixed threshold.
Gaussian Fourier smoothing, expressed against the probability law N(0,2).
Integrating the scaled CF defects gives the Gaussian integral limit.
The positive finite smoothing constant; no Gamma evaluation is needed.
Equations
Instances For
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.