All Tables

Table 1: Parameters for the optimized orbitals.
Table 2: Comparisons of fine-structure energy levels (in cm^-1) for K VIII. CSS: measurement of Churilov et al. (1989); NIST: (http://www.nist.gov); CFF: calculation by Fischer (2002) and BF: calculation by Fawcett (1983). (a) and (b) in the present calculation represents fine-tuned and ab initio energies respectively.
Table 3: Comparisons of fine-structure energy levels (in cm^-1) for Ti XI. CSS; measurement of Churilov et al. (1989); NIST: (http://www.nist.gov); CFF: calculation by Fischer (2002) and BF: calculation by Fawcett (1983). (a) and (b) in the present calculation represents fine-tuned and ab initio energies respectively.
Table 4: Oscillator strengths for some dipole-allowed transitions, $f_{\rm L}$ and $f_{\rm V}$ are the present length and velocity forms. OT represents other calculations.
Table 5: Lifetimes $(\rm 10^{-9}s)$ for some long-lived levels of K VIII and Ti XI. Superscripts a-e represent the same authors as in Table 4.
Table 6: Oscillator strengths ( $f_{\rm L}$ and $f_{\rm V}$ ), transition probabilities ( $A_{\rm L}$ ) and line strengths (LST) for allowed and intercombination transitions of K⁷⁺ among levels of n=3 complex. I and J are initial and final state of the transition as labeled in "Index'' column in Table 2.
Table 7: Oscillator strengths ( $f_{\rm L}$ and $f_{\rm V}$ ), transition probabilities ( $A_{\rm L}$ ) and line strengths (LST) for allowed and intercombination transitions in Ti¹⁰⁺ among its levels of n=3 complex. I and J are initial and final states of the transition as labeled under the "Index'' column in Table 3.