The hyperfine structure parameters of the 1s22snp (n=2, 3) 3P states for the beryllium isoelectronic sequence from Z= 4 to 10 are calculated with the full-core plus correlation (FCPC) wave functions. For the 1s22s2p 3P state of the beryllium atom, the calculated fine structure parameters are in good agreement with the latest theoretical and experimental data in the literature. It is shown that hyperfine constants of the low-lying excited states for the beryllium atom can be calculated accurately using this theoretical method. For 1s22snp (n=2, 3) 3P states of the beryllium isoelectronic sequence, our predictions may provide valuable reference data for other theoretical calculations and experimental measurements in future
$^{1}$H. Odabasi, J. Opt. Soc. Am. 59, 583 (1969).Author Institution: National Bureau of StandardsTh...
https://journals.aps.org/pra/abstract/10.1103/PhysRevA.100.032504Benchmark calculations of the total...
The hyperfine-induced 2s2p {sup 3}P{sub 0}-2s{sup 2} {sup 1}S{sub 0} transition rate for Be-like {su...
The recently presented general algorithm for calculating an atomic fine structure [Kȩdziorski et al....
We report on the calibration and absolute frequency results for the 2s2p1P1 state in neutral atomic ...
Multiconfiguration Hartree-Fock (MCHF) calculations of hyperfine constants for the 2s2p 3P states of...
Energy levels, hyperfine interaction constants, and Landé gJ-factors are reported for n=2 states in ...
The ground and a few excited states of the beryllium atom in external uniform magnetic fields are ca...
The high precision relativistic and radiative corrections to the energy of the excited 3 S-1 state o...
The two lowest bound excited states of the Be− ion, 1s2 2s2p24P and 1s2 2p34S0, and their respective...
Author Institution: Laboratory of Chemical Physics, California Institute of TechnologyMulticonfigura...
The low-lying valence levels of BeO, are calculated by the LCAO MO SCF method in order to ascertain ...
Energy levels, hyperfine interaction constants, and Landé gJ -factors are reported for n = 2 states ...
Benchmark calculations of the total and transition energies of the four lowest S-1 states of the ber...
[[sponsorship]]原子與分子科學研究所[[note]]已出版;[SCI];有審查制度;具代表性[[note]]http://gateway.isiknowledge.com/gateway...
$^{1}$H. Odabasi, J. Opt. Soc. Am. 59, 583 (1969).Author Institution: National Bureau of StandardsTh...
https://journals.aps.org/pra/abstract/10.1103/PhysRevA.100.032504Benchmark calculations of the total...
The hyperfine-induced 2s2p {sup 3}P{sub 0}-2s{sup 2} {sup 1}S{sub 0} transition rate for Be-like {su...
The recently presented general algorithm for calculating an atomic fine structure [Kȩdziorski et al....
We report on the calibration and absolute frequency results for the 2s2p1P1 state in neutral atomic ...
Multiconfiguration Hartree-Fock (MCHF) calculations of hyperfine constants for the 2s2p 3P states of...
Energy levels, hyperfine interaction constants, and Landé gJ-factors are reported for n=2 states in ...
The ground and a few excited states of the beryllium atom in external uniform magnetic fields are ca...
The high precision relativistic and radiative corrections to the energy of the excited 3 S-1 state o...
The two lowest bound excited states of the Be− ion, 1s2 2s2p24P and 1s2 2p34S0, and their respective...
Author Institution: Laboratory of Chemical Physics, California Institute of TechnologyMulticonfigura...
The low-lying valence levels of BeO, are calculated by the LCAO MO SCF method in order to ascertain ...
Energy levels, hyperfine interaction constants, and Landé gJ -factors are reported for n = 2 states ...
Benchmark calculations of the total and transition energies of the four lowest S-1 states of the ber...
[[sponsorship]]原子與分子科學研究所[[note]]已出版;[SCI];有審查制度;具代表性[[note]]http://gateway.isiknowledge.com/gateway...
$^{1}$H. Odabasi, J. Opt. Soc. Am. 59, 583 (1969).Author Institution: National Bureau of StandardsTh...
https://journals.aps.org/pra/abstract/10.1103/PhysRevA.100.032504Benchmark calculations of the total...
The hyperfine-induced 2s2p {sup 3}P{sub 0}-2s{sup 2} {sup 1}S{sub 0} transition rate for Be-like {su...