Two-dimensional relativistic hydrogenic atoms: A complete set of constants of motion

Abstract

The complete set of operators commuting with the Dirac Hamiltonian and exact analytic solution of the Dirac equation for the two-dimensional Coulomb potential is presented. Beyond the eigenvalue μ of the operator jz, two quantum numbers η and are introduced as eigenvalues of hermitian operators P=βσz' and K=β(σz'lz+1/2), respectively. The classification of states according to the full set of constants of motion without referring to the non-relativistic limit is proposed. The linear Paschen-Back effect is analyzed using exact field-free wave-functions as a zero-order approximation.

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