Lemma 6.2 (zero-mass logarithmic energy) for the truncated kernel #
We work with explicit "atoms": a finite family of continuous curves γ k : ℝ → ℂ
(parametrised over [0, 2π]) with real weights s k. The double integral of a kernel f
against the atoms k, l is pairInt γ f k l, and the energy is
energy s γ f = ∑ k l, s k * s l * pairInt γ f k l.
For the truncated kernel Ltr a b r = (1/2) ∫_a^b (e^{-s} - e^{-s r²})/s ds and zero total mass
∑ s k = 0, the energy is nonpositive (energy_Ltr_nonpos): this is the Gaussian
positivity argument of the paper.
Integrability of a Gaussian on ℂ.
Fubini between an interval integral and an integral over ℂ, for a continuous integrand
with a Gaussian bound in the complex variable.
The truncated kernel #
Continuity of the Gaussian pair integral in the parameter.
The truncated-kernel pair integral in terms of Gaussian pair integrals.
Lemma 6.2 for the truncated kernel: the energy of a zero-mass combination of atoms
with respect to L_{a,b} is nonpositive.