Elementary commutator method for the Dirac equation with long-range perturbations
Shinichi Arita, Kenichi Ito
TL;DR
This work develops an elementary commutator framework for the Dirac operator with long-range perturbations in $\mathbb{R}^d$, using the generator of radial translations as the conjugate operator. It proves Rellich’s theorem in optimally weighted Agmon–Hörmander spaces $\mathcal{B}^*_0$, establishes locally uniform LAP bounds between Besov-type spaces, and, under a massless assumption, derives algebraic and analytic radiation conditions including Sommerfeld-type uniqueness. The approach avoids energy cutoffs, pseudodifferential calculus, or Schrödinger reduction, relying instead on precise first-order commutator estimates and carefully chosen weight functions $\Theta$ built from $f=\chi(|x|)+|x|(1-\chi(|x|))$. The results lay a rigorous foundation for the stationary scattering theory of long-range Dirac operators and provide tools for analysing resolvent limits and radiation behavior at infinity. Overall, the paper contributes a self-contained, elementary pathway to comprehensive spectral and scattering results for Dirac operators with long-range perturbations, with potential applications to relativistic quantum scattering and electromagnetic/mass perturbations in arbitrary dimension.$
Abstract
We present direct and elementary commutator techniques for the Dirac equation with long-range electric and mass perturbations. The main results are absence of generalized eigenfunctions and locally uniform resolvent estimates, both in terms of the optimal Besov-type spaces. With an additional massless assumption, we also obtain an algebraic radiation condition of projection type. For their proofs, following the scheme of Ito-Skibsted, we adopt, along with various weight functions, the generator of radial translations as conjugate operator, and avoid any of advanced functional analysis, pseudodifferential calculus, or even reduction to the Schrödinger equation. The results of the paper would serve as a foundation for the stationary scattering theory of the Dirac operator.
