Relativistic effects strongly influence the nuclear quadrupole coupling of atoms, molecules or solids. As first shown by Casimir in 1936, in the atomic or single-centre case, for the two states j=l±s, three radial electric-field-gradient (EFG) integrals, R++,R+−, and R, must be introduced. The relativistic correction factors, defined for operator \documentclass[12pt]{minimal}
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