Diffraction for the Dirac–Coulomb Propagator

Dean Baskin, Jared Wunsch*

*Corresponding author for this work

Research output: Contribution to journalArticlepeer-review

Abstract

The Dirac equation in R1 , 3 with potential Z/ r is a relativistic field equation modeling the hydrogen atom. We analyze the singularity structure of the propagator for this equation, showing that the singularities of the Schwartz kernel of the propagator are along an expanding spherical wave away from rays that miss the potential singularity at the origin, but also may include an additional spherical wave of diffracted singularities emanating from the origin. This diffracted wavefront is 1 - ϵ derivatives smoother than the main singularities, for all ϵ> 0 , and is a conormal singularity.

Original languageEnglish (US)
Pages (from-to)2607-2659
Number of pages53
JournalAnnales Henri Poincare
Volume24
Issue number8
DOIs
StatePublished - Aug 2023

Funding

The authors are grateful to Christian Gérard and Michał Wrochna for suggesting the problem and providing helpful insight into its importance, as well as for helpful comments on an early version of the manuscript. They are also grateful to Richard Melrose, András Vasy, and especially Oran Gannot for many helpful conversations. Two anonymous referees made a number of corrections and suggestions that improved the presentation. The research for this paper began during a Research in Paris stay at the Institut Henri Poincaré. Part of this material is based upon work supported by the National Science Foundation under Grant No. DMS-1440140 while the authors were in residence at the Mathematical Sciences Research Institute in Berkeley, California, during the Fall 2019 semester. DB was supported by NSF CAREER grant DMS-1654056. JW was supported by NSF grant DMS-1600023 and Simons Foundation Grant 631302.

ASJC Scopus subject areas

  • Statistical and Nonlinear Physics
  • Nuclear and High Energy Physics
  • Mathematical Physics

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