1991
DOI: 10.1103/physreva.44.1773
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Spin-orbit effects in the heavy alkaline-earth atoms

Abstract: Complex bound and autoionizing spectra of strontium, barium, and radium are treated at two different levels of approximation using multichannel-quantum-defect techniques (MQDT) and eigenchannel R-matrix calculations. In the first level, the R-matrix calculations are conducted entirely in LS coupling without explicitly including any spin-orbit terms in the Hamiltonian.A subsequent frame transformation to jj coupling is then carried out prior to the MQDT treatment. In the second level, the entire R-matrix calcul… Show more

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Cited by 133 publications
(114 citation statements)
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“…However, the use of a polarization potential tuned to the experimental binding energy will implicitly take into account the influence of relativistic effects upon the core electron distribution. Further, Greene and Aymar have shown that the spin-orbit interaction does not have major effect on the structure of the alkaline-earth-metal wave functions [15].…”
Section: A Methodologymentioning
confidence: 99%
“…However, the use of a polarization potential tuned to the experimental binding energy will implicitly take into account the influence of relativistic effects upon the core electron distribution. Further, Greene and Aymar have shown that the spin-orbit interaction does not have major effect on the structure of the alkaline-earth-metal wave functions [15].…”
Section: A Methodologymentioning
confidence: 99%
“…The same theoretical and numerical techniques have been used as in our previous articles [1,3,4]. The techniques are "nearly" ab initio; effects of the 18 core electrons are described using a screened Coulomb potential [5] with a dipole polarizability that gives the correct energies of the one-electron-like ion Sc III. We solve for the three-electron valence wave function with the streamlined version [6] of the eigenchannel B-matrix technology in an A-matrix volume rq, r2, r3 ( 21 a.u.…”
Section: Introductionmentioning
confidence: 99%
“…At high n, the 5sns 1 S 0 Rydberg series is only weakly perturbed [44,46], and the relevant dipole matrix elements can be calculated using a single active electron treatment. We calculated two independent sets of van der Waals C 6 coefficients using wavefunctions obtained from single-electron model-potential calculations [30] (circles in figure 5) and from twoelectron Hartree-Fock calculations using the effective Sr 2+ core potential of [47]. As shown in figure 4 both approaches yield nearly identical C 6 values, which over the depicted range are well described by the simple fit-formula For a given n the magnitude of the C 6 coefficients is comparable to that for Rb(ns) states.…”
Section: Rydberg-rydberg Atom Interactionsmentioning
confidence: 99%