Abstract. We present highly correlated multi-configuration Hartree-Fock (MCHF) calculations of the hyperfine structure of the 3p5 2P oJ levels of 33S − and 35,37Cl. We obtain a good agreement with observation. The hyperfine structure of the neutral sulfur 33S 3p4 3PJ lowest multiplet that has never been measured to the knowledge of the authors, is also estimated theoretically. We discuss some interesting observations made on the description of the atomic core in MCHF theory
We calculated hyperfine structure constants of the 5d6s(2), 5d(2)6s, 5d(3), 5d(2)7s, 5d6s7s, 5d6p(2)...
In the frame of the effective-operator technique applied to atomic hyperfine structure in the lNl' c...
Hyperfine structure parameters are calculated for the 2p2(3P)3s 4PJ, 2p2(3P)3p 4PoJ and2p2(3P)3p 4Do...
Recent multi-configuration Hartree-Fock (MCHF) calculations of atomic hyperfine structures are revie...
Multiconfiguration Hartree-Fock (MCHF) and multiconfiguration Dirac-Hartree-Fock (MCDHF) calculation...
Multiconfiguration Hartree-Fock (MCHF) calculations of hyperfine constants for the 2s2p 3P states of...
Accurate hyperfine-structure parameters for the ground and first excited states of lithium are repor...
We are interested in complex electronic structures of various atomic and ionics systems. We use an a...
A historical review of the early development of Hartree-Fock and Multiconfiguration Hartree-Fock the...
The multi-configuration Dirac-Fock method has been employed to calculate the magnetic dipole hyperfi...
Accurate results for hyperfine structure (HFS) constants of (d + s)n states often require the inclus...
Hyperfine structure constants for the ground and first excited states of sodium are calculated using...
For the first time a spin-polarized extended Hartree-Fock calculation on a three-electron system, Li...
The hyperfine-structure of the 3p 4D and 3d 4F° levels of 14NIII has been studied by the beam-foil t...
Calculations on the hyperfine-splitting constants for the atoms B, C, N, O, and F have been carried ...
We calculated hyperfine structure constants of the 5d6s(2), 5d(2)6s, 5d(3), 5d(2)7s, 5d6s7s, 5d6p(2)...
In the frame of the effective-operator technique applied to atomic hyperfine structure in the lNl' c...
Hyperfine structure parameters are calculated for the 2p2(3P)3s 4PJ, 2p2(3P)3p 4PoJ and2p2(3P)3p 4Do...
Recent multi-configuration Hartree-Fock (MCHF) calculations of atomic hyperfine structures are revie...
Multiconfiguration Hartree-Fock (MCHF) and multiconfiguration Dirac-Hartree-Fock (MCDHF) calculation...
Multiconfiguration Hartree-Fock (MCHF) calculations of hyperfine constants for the 2s2p 3P states of...
Accurate hyperfine-structure parameters for the ground and first excited states of lithium are repor...
We are interested in complex electronic structures of various atomic and ionics systems. We use an a...
A historical review of the early development of Hartree-Fock and Multiconfiguration Hartree-Fock the...
The multi-configuration Dirac-Fock method has been employed to calculate the magnetic dipole hyperfi...
Accurate results for hyperfine structure (HFS) constants of (d + s)n states often require the inclus...
Hyperfine structure constants for the ground and first excited states of sodium are calculated using...
For the first time a spin-polarized extended Hartree-Fock calculation on a three-electron system, Li...
The hyperfine-structure of the 3p 4D and 3d 4F° levels of 14NIII has been studied by the beam-foil t...
Calculations on the hyperfine-splitting constants for the atoms B, C, N, O, and F have been carried ...
We calculated hyperfine structure constants of the 5d6s(2), 5d(2)6s, 5d(3), 5d(2)7s, 5d6s7s, 5d6p(2)...
In the frame of the effective-operator technique applied to atomic hyperfine structure in the lNl' c...
Hyperfine structure parameters are calculated for the 2p2(3P)3s 4PJ, 2p2(3P)3p 4PoJ and2p2(3P)3p 4Do...