Energy levels, specific mass shift parameters, hyperfine interaction constants, Landé gJ factors, and transition probabilities between computed levels are reported for C II, N III, and O IV. Results include levels belonging to 2s22p,2s2p2,2p3,2s23s,2s23p,2s23d,2s2p3s and, in the case of C II, the 2s24s and 2s24p configurations. Wavefunctions were determined using the multiconfiguration Dirac–Hartree–Fock method and account for valence, core–valence, and core–core correlation effects
Relativistic configuration interaction hyperfine constants (HFC) have been obtained for all 5[Formul...
The hyperfine coupling constant for the nitrogen atom is evaluated by large-scale MRD-CI calculation...
The bottom three J = 1 K II levels are nearly degenerate, leading to strong interactions among them,...
Energy levels, fine-structure separations, specific mass shift parameters, isotope shifts, hyperfine...
Energies, electric dipole, magnetic dipole, and electric quadrupole transition rates, hyperfine stru...
The mass shift parameters, the electron density at the origin, the hyperfine interaction constants ...
Energy levels, hyperfine interaction constants, and Landé gJ -factors are reported for n = 2 states ...
Extensive multiconfiguration Dirac-Hartree-Fock (MCDHF) calculations and relativistic configuration ...
Extensive multiconfiguration Dirac-Hartree-Fock (MCDHF) calculations and relativistic configuration ...
Energy levels, normal and specific mass shift parameters as well as electronic densities at the nucl...
Energy levels, normal and specific mass shift parameters as well as electronic densities at the nucl...
Multiconfiguration Hartree-Fock (MCHF) and multiconfiguration Dirac-Hartree-Fock (MCDHF) calculation...
Energy levels, hyperfine interaction constants, and Landé gJ-factors are reported for n=2 states in ...
Based on relativistic wavefunctions from multiconfiguration Dirac–Hartree–Fock and configuration in...
Our relativistic configuration-interaction (RCI) methodology has been extended to multireference cas...
Relativistic configuration interaction hyperfine constants (HFC) have been obtained for all 5[Formul...
The hyperfine coupling constant for the nitrogen atom is evaluated by large-scale MRD-CI calculation...
The bottom three J = 1 K II levels are nearly degenerate, leading to strong interactions among them,...
Energy levels, fine-structure separations, specific mass shift parameters, isotope shifts, hyperfine...
Energies, electric dipole, magnetic dipole, and electric quadrupole transition rates, hyperfine stru...
The mass shift parameters, the electron density at the origin, the hyperfine interaction constants ...
Energy levels, hyperfine interaction constants, and Landé gJ -factors are reported for n = 2 states ...
Extensive multiconfiguration Dirac-Hartree-Fock (MCDHF) calculations and relativistic configuration ...
Extensive multiconfiguration Dirac-Hartree-Fock (MCDHF) calculations and relativistic configuration ...
Energy levels, normal and specific mass shift parameters as well as electronic densities at the nucl...
Energy levels, normal and specific mass shift parameters as well as electronic densities at the nucl...
Multiconfiguration Hartree-Fock (MCHF) and multiconfiguration Dirac-Hartree-Fock (MCDHF) calculation...
Energy levels, hyperfine interaction constants, and Landé gJ-factors are reported for n=2 states in ...
Based on relativistic wavefunctions from multiconfiguration Dirac–Hartree–Fock and configuration in...
Our relativistic configuration-interaction (RCI) methodology has been extended to multireference cas...
Relativistic configuration interaction hyperfine constants (HFC) have been obtained for all 5[Formul...
The hyperfine coupling constant for the nitrogen atom is evaluated by large-scale MRD-CI calculation...
The bottom three J = 1 K II levels are nearly degenerate, leading to strong interactions among them,...