$L^p$ Asymptotics of the Möbius Energy Density of Helix Curves

Abstract

Motivated by the recent work of Lipton on the Möbius energy of helix curves, we extend the study to the $L^p$ asymptotics of the meromorphic family \[ M_ρ(t) = \frac{ρ^2+1}{ρ^2 t^2 + 4 \sin^2(t/2)} - \frac{1}{t^2}. \] The helix has infinite Möbius energy, but the arclength-rescaled energy density is finite. As $ρ\to 0$ the helix coils infinitely tight. Using contour integration and a careful Laurent expansion near the poles, we establish $I_p(ρ) := \left(\int_{-\infty}^\infty M_ρ(t)^p \, dt\right)^{1/p} \sim C_p \, ρ^{-(2-1/p)} $ for integer $p > 1$, extended to real $p > 1$, where $C_p$ is an explicit constant involving $ζ(2p-1)$. The result gives the precise $L^p$ blowup rate of the Möbius energy density as the pitch $ρ\to 0$. The borderline case $p=1$ yields a logarithmic correction $I_1(ρ) \sim \log(1/ρ)/ρ$, recovering Lipton's main theorem. We derive a quantitative coiling barrier. Numerical verification confirms the scaling exponent to high precision.