Abstract

A relativistic Fock-space coupled cluster theory based on the Dirac—Coulomb—Breit wavefunctions has been developed and implemented, employing analytic basis sets of Gaussian-type functions. Relativistic all-order calculations including single and double excitations were performed for the ground states of the He and Be atoms and for the Ne ( Z = 10), Ar ( Z = 18) and Sn ( Z = 50) ions with 2–5 electrons. Comparison is made with the Dirac—Coulomb and non-relativistic formulation and with available experimental results. The non-additivity of relativistic and correlation effects is discussed.

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