A version of the configuration interaction method, which has been recently developed to deal with large number of valence electrons, has been used to calculate magnetic dipole and electric quadrupole hyperfine structure constants for a number of states of erbium and fermium. Calculations for fermium are done for extracting nuclear moments of Fm isotopes from recent and future measurements. Calculations for erbium, which has electronic structure similar to those of fermium, are done to study the accuracy of the method.Comment: 4 pages, no figures. arXiv admin note: text overlap with arXiv:2301.0315
Vacuum polarization, nuclear structure and recoil, radiative corrections to the hyperfine structure ...
Becke and Edgecombe suggested in 1990 a theoretical tool to describe electron localization in atoms ...
Hyperfine structure (HFS) of atomic energy levels arises due to interactions of atomic electrons wit...
We carried out calculations of the energies and magnetic dipole hyperfine structure constants of the...
Hyperfine structure of the ground rotational level of the metastable $^3\Delta_1$ electronic state o...
Within the nuclear DFT approach, we determined the magnetic dipole and electric quadrupole moments f...
Calculations of the magnetic hyperfine structure rely on the input of nuclear properties - nuclear m...
Nuclear structure of 156,158Dy isotopes have been studied in the frame work of the interacting boson...
We report measurements of the hyperfine coupling constant for the $8p \ ^2P_{1/2}$ level of atomic c...
We calculate the Schiff moments of the nuclei 199Hg and 211Ra in completely self-consistent odd-nucl...
There is strong interest in atomic and nuclear physics to the study of superheavy elements by the se...
The de Haas-van Alphen (dHvA) effect is one of the most powerful and straightforward methods of dete...
Ultracold molecules with both electron spin and an electric dipole moment offer new possibilities in...
The hyperfine structure splitting in the 6p2 4S3/2 -> 6p27s 4P1/2 transition at 307 nm in atomic 208...
As known, electron vacuum polarization by nuclear Coulomb field produces Uehling potential with the ...
Vacuum polarization, nuclear structure and recoil, radiative corrections to the hyperfine structure ...
Becke and Edgecombe suggested in 1990 a theoretical tool to describe electron localization in atoms ...
Hyperfine structure (HFS) of atomic energy levels arises due to interactions of atomic electrons wit...
We carried out calculations of the energies and magnetic dipole hyperfine structure constants of the...
Hyperfine structure of the ground rotational level of the metastable $^3\Delta_1$ electronic state o...
Within the nuclear DFT approach, we determined the magnetic dipole and electric quadrupole moments f...
Calculations of the magnetic hyperfine structure rely on the input of nuclear properties - nuclear m...
Nuclear structure of 156,158Dy isotopes have been studied in the frame work of the interacting boson...
We report measurements of the hyperfine coupling constant for the $8p \ ^2P_{1/2}$ level of atomic c...
We calculate the Schiff moments of the nuclei 199Hg and 211Ra in completely self-consistent odd-nucl...
There is strong interest in atomic and nuclear physics to the study of superheavy elements by the se...
The de Haas-van Alphen (dHvA) effect is one of the most powerful and straightforward methods of dete...
Ultracold molecules with both electron spin and an electric dipole moment offer new possibilities in...
The hyperfine structure splitting in the 6p2 4S3/2 -> 6p27s 4P1/2 transition at 307 nm in atomic 208...
As known, electron vacuum polarization by nuclear Coulomb field produces Uehling potential with the ...
Vacuum polarization, nuclear structure and recoil, radiative corrections to the hyperfine structure ...
Becke and Edgecombe suggested in 1990 a theoretical tool to describe electron localization in atoms ...
Hyperfine structure (HFS) of atomic energy levels arises due to interactions of atomic electrons wit...