Electronic structure of Rydberg atoms in parallel electric and magnetic fields

David Farrelly, T. Uzer, Paul E. Raines, Joel P. Skelton, and John A. Milligan
Phys. Rev. A 45, 4738 – Published 1 April 1992
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Abstract

The structure of the eigenstates of a hydrogen atom in parallel uniform electric and magnetic fields is investigated using high-order classical perturbation theory. The Kustaanheimo-Stiefel transformation is first used to convert the problem into an anharmonically perturbed four-dimensional isotropic oscillator. A canonical transformation to a set of extended ‘‘Lissajous’’ action-angle variables is then introduced that considerably simplifies the perturbation expansion, leading to a simple and compelling classification scheme for the eigenstates. Extended Lissajous action-angle variables allow the construction of rotational energy surfaces, which provide a compact geometrical picture that captures important details of the energy-level structure of the system.

  • Received 17 October 1991

DOI:https://doi.org/10.1103/PhysRevA.45.4738

©1992 American Physical Society

Authors & Affiliations

David Farrelly

  • Institute for Theoretical Physics, University of California, Santa Barbara, California 93106-4030
  • Department of Chemistry and Biochemistry, Utah State University, Logan, Utah 84322-0300

T. Uzer

  • Institute for Theoretical Physics, University of California, Santa Barbara, California 93106-4030
  • School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332-0430

Paul E. Raines and Joel P. Skelton

  • School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332-0430

John A. Milligan

  • Department of Chemistry and Biochemistry, University of California, Los Angeles, California 90024-1569
  • Department of Chemistry and Biochemistry, Utah State University, Logan, Utah 84322-0300

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Vol. 45, Iss. 7 — April 1992

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