corner
corner

Phys. Rev. A 79, 032511 (2009) [11 pages]

Correlation and relativistic effects for the 4f-nl multipole transitions in Yb III ions

Download: PDF (138 kB) Buy this article Export: BibTeX or EndNote (RIS)

U. I. Safronova1,2 and M. S. Safronova3
1Physics Department, University of Nevada, Reno, Nevada 89557, USA
2Institute of Spectroscopy, Russian Academy of Science, Troitsk, Moscow, Russia
3Department of Physics and Astronomy, 217 Sharp Lab, University of Delaware, Newark, Delaware 19716, USA

Received 21 December 2008; published 19 March 2009

Wavelengths, transition rates, and line strengths are calculated for the multipole (E1, M1, E2, M2, and E3) transitions between the excited [Xe]4f13ns, [Xe]4f13nd, and [Xe]4f13np and the ground [Xe]4f14 state in Yb III ion with the nuclear charge Z=70 ([Xe]=[Ni]4s24p64d105s25p6). Relativistic many-body perturbation theory (RMBPT), including the Breit interaction, is used to evaluate energies and transition rates for multipole transitions in this hole-particle system. This method is based on the relativistic many-body perturbation theory that agrees with multiconfiguration Dirac-Fock calculations in lowest-order, includes all second-order correlation corrections, and includes corrections from negative energy states. The calculations start from a [Xe]4d14 Dirac-Fock potential. First-order perturbation theory is used to obtain intermediate-coupling coefficients, and second-order RMBPT is used to determine the matrix elements. Evaluated multipole matrix elements for transitions from excited states into the ground states and transitions between excited states are used to determine the lifetime of the 20 [Xe]4f135d(J) levels, four [Xe]4f136s(J) levels, 12 [Xe]4f136p(J) levels, and four [Xe]4f137s(J) levels.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevA.79.032511
DOI:
10.1103/PhysRevA.79.032511
PACS:
31.15.ac, 31.15.ag, 31.15.aj