Relativistic distorted-wave collision strengths and oscillator strengths for the 185Δn=0 transitions with n=2n=2 in the 67 C-like ions with 26≤Z≤9226≤Z≤92

Abstract Relativistic distorted-wave collision strengths have been calculated for the 185 Δn=0Δn=0 transitions with n=2n=2 in the 67 C-like ions with nuclear charge number ZZ in the range 26≤Z≤9226≤Z≤92. The calculations were made for the six final, or scattered, electron energies E′=0.03,0.08,0.20,0.42,0.80,  and  1.40E′=0.03,0.08,0.20,0.42,0.80,  and  1.40, where E′E′ is in units of Zeff2 Ry with Zeff=Z−4.17. In addition, electric dipole oscillator strengths are provided. In the present collision-strength calculations, an improved “top-up” method, which employs relativistic plane waves, was used to obtain the high partial-wave contribution for each transition, in contrast to the partial-relativistic Coulomb–Bethe approximation used in previous work by Zhang and Sampson [H.L. Zhang, D.H. Sampson, At. Data Nucl. Data Tables 63 (1996) 275]. In that earlier work, collision strengths were also provided for the same 185 Δn=0Δn=0 transitions in C-like ions, but for the more limited list of 46 ions with ZZ in the range 9≤Z≤549≤Z≤54. The collision strengths covered in the present work, particularly those for optically allowed transitions, should be more accurate than the corresponding data given by Zhang and Sampson [H.L. Zhang, D.H. Sampson, At. Data Nucl. Data Tables 63 (1996) 275] and are presented here to replace those earlier results.