Lifetimes of different hyperfine levels of 3d⁹4s ³D₃, <em>τ_F</em>, relative to the lifetime of 3d⁹4s ³D₃ which decays by the pure M3 transition, <em>τ_M3</em>

Abstract

<p><strong>Figure 2.</strong> Lifetimes of different hyperfine levels of 3d⁹4s ³D₃, <em>τ_F</em>, relative to the lifetime of 3d⁹4s ³D₃ which decays by the pure M3 transition, <em>τ_M3</em>. Results for all hyperfine levels of different isotopes in table <a href="http://iopscience.iop.org/0953-4075/46/14/145001/article#b467799t4" target="_blank">4</a> are presented.</p> <p><strong>Abstract</strong></p> <p>Based on the multi-configuration Dirac–Hartree–Fock method and using the GRASPVU package, a theoretical investigation was performed to study the lifetimes of hyperfine levels of the first excited level 3d⁹4s ³D₃ in Ni-like ions (<em>Z</em> = 72–79) for all stable isotopes with nuclear spin. Comparisons between hyperfine-induced electric quadrupole transition rates and the pure magnetic octupole transition rates show that the extra electric quadrupole transition channel caused by the nuclear magnetic dipole and electric quadrupole hyperfine interaction is important for most hyperfine levels in each individual ion. Lifetimes of most hyperfine levels are sensitive to this extra decay channel. Extreme cases are found in ¹⁸¹Ta, ¹⁸⁵Re and ¹⁸⁷Re, where lifetimes of some hyperfine levels are shortened by more than an order of magnitude.</p