Energies of np (n=6-9), ns (n=7-9), nd (n=6-8), and nf (n=5-6) states in Tl I and Pb II are obtained using relativistic many-body perturbation theory. Reduced matrix elements, oscillator strengths, transition rates, and lifetimes are determined for the 72 possible electric-dipole transitions. Electric-quadrupole and magnetic-dipole matrix elements are evaluated to obtain np(3/2) - mp(1/2) (n,m=6,7) transition rates. Hyperfine constants A are evaluated for a number of states in 205Tl. First-, second-, third-, and all-order corrections to the energies and matrix elements and first- and second-order Breit corrections to energies are calculated. In our implementation of the all-order method, single and double excitations of Dirac-Fock wave func...
An extensive set of level energies, wavelengths, line strengths, oscillator strengths, lifetimes, hy...
Abstract. A relativistic many-body method is devel-oped to calculate energy and transition rates for...
Transition rates, oscillator strengths, and line strengths are calculated for electric-dipole (E1) t...
The energies of the ground np states and the lowest ns and nd states in neutral B, Al, Ga, In and Tl...
The excitation energies of ns, np, nd, and nf n6 states in neutral lithium are evaluated within the...
Excitation energies of ns, np, nd, and nf (n ≤ 6) states in neutral lithium are evaluated within the...
Energy levels of 30 low-lying states of Lu2+ and allowed electric-dipole matrix elements between the...
Energies of 5l_j (l= s, p, d, f, g) and 4f_j states in neutral Ag and Ag-like ions with nuclear char...
Excitation energies for 2l-3l′ hole-particle states of Ne-like ions are determined to second order i...
A systematic way of simultaneously handling relativistic and many-body effects for electric dipole t...
Extensive self-consistent multi-configuration Dirac-Fock(MCDF) calculations and second-order many- b...
We calculated relativistic energies and Landéfactors for 5d6s², 5d²6s, 5d³, 5d6s7s, 4f6s6p, 5d6s6p, ...
Extensive self-consistent multi-configuration Dirac-Foci (MCDF) calculations and second-order many b...
Energy levels and oscillator strengths for electric-dipole (E1), electric-quadrupole (E2), magnetic-...
We calculated relativistic energies and Lande factors for 5d6s(2) 5d(2)6s, 5d(3), 5d6s7s, 4f6s6p, 5d...
An extensive set of level energies, wavelengths, line strengths, oscillator strengths, lifetimes, hy...
Abstract. A relativistic many-body method is devel-oped to calculate energy and transition rates for...
Transition rates, oscillator strengths, and line strengths are calculated for electric-dipole (E1) t...
The energies of the ground np states and the lowest ns and nd states in neutral B, Al, Ga, In and Tl...
The excitation energies of ns, np, nd, and nf n6 states in neutral lithium are evaluated within the...
Excitation energies of ns, np, nd, and nf (n ≤ 6) states in neutral lithium are evaluated within the...
Energy levels of 30 low-lying states of Lu2+ and allowed electric-dipole matrix elements between the...
Energies of 5l_j (l= s, p, d, f, g) and 4f_j states in neutral Ag and Ag-like ions with nuclear char...
Excitation energies for 2l-3l′ hole-particle states of Ne-like ions are determined to second order i...
A systematic way of simultaneously handling relativistic and many-body effects for electric dipole t...
Extensive self-consistent multi-configuration Dirac-Fock(MCDF) calculations and second-order many- b...
We calculated relativistic energies and Landéfactors for 5d6s², 5d²6s, 5d³, 5d6s7s, 4f6s6p, 5d6s6p, ...
Extensive self-consistent multi-configuration Dirac-Foci (MCDF) calculations and second-order many b...
Energy levels and oscillator strengths for electric-dipole (E1), electric-quadrupole (E2), magnetic-...
We calculated relativistic energies and Lande factors for 5d6s(2) 5d(2)6s, 5d(3), 5d6s7s, 4f6s6p, 5d...
An extensive set of level energies, wavelengths, line strengths, oscillator strengths, lifetimes, hy...
Abstract. A relativistic many-body method is devel-oped to calculate energy and transition rates for...
Transition rates, oscillator strengths, and line strengths are calculated for electric-dipole (E1) t...