# Relativistic distorted-wave collision strengths for the 49 Δn=0 optically allowed transitions with n=2 in the 67 B-like ions with 26≤Z≤92

## Abstract

Relativistic distorted-wave collision strengths have been calculated for the 49 Δn=0 optically allowed transitions with n=2 in the 67 B-like ions with nuclear charge number Z in the range 26≤Z≤92. The calculations were made for the four final, or scattered, electron energies E{sup ′}=0.20, 0.42, 0.80, and 1.40, where E{sup ′} is in units of Z{sub eff}{sup 2} Ry with Z{sub eff}=Z−3.33. In the present 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 and D.H. Sampson, At. Data Nucl. Data Tables 56 (1994) 41]. In that earlier work, collision strengths were also provided for B-like ions, but for a more comprehensive data set consisting of all 105 Δn=0 transitions, six scattered energies and the 85 ions with Z in the range 8≤Z≤92. The collision strengths covered in the present work should be more accurate than the corresponding data given by Zhang and Sampson [H.L. Zhang and D.H. Sampson, At. Data Nucl. Data Tables 56 (1994) 41] and are presented here to replace those earlier results.

- Authors:

- Publication Date:

- OSTI Identifier:
- 22314846

- Resource Type:
- Journal Article

- Journal Name:
- Atomic Data and Nuclear Data Tables

- Additional Journal Information:
- Journal Volume: 100; Journal Issue: 3; Other Information: Copyright (c) 2014 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA); Journal ID: ISSN 0092-640X

- Country of Publication:
- United States

- Language:
- English

- Subject:
- 73 NUCLEAR PHYSICS AND RADIATION PHYSICS; APPROXIMATIONS; DISTORTED WAVE THEORY; ELECTRONS; ENERGY-LEVEL TRANSITIONS; ION COLLISIONS; MULTICHARGED IONS; PARTIAL WAVES; RELATIVISTIC RANGE; WAVE PROPAGATION

### Citation Formats

```
Fontes, Christopher J., E-mail: cjf@lanl.gov, and Zhang, Hong Lin.
```*Relativistic distorted-wave collision strengths for the 49 Δn=0 optically allowed transitions with n=2 in the 67 B-like ions with 26≤Z≤92*. United States: N. p., 2014.
Web. doi:10.1016/J.ADT.2013.09.001.

```
Fontes, Christopher J., E-mail: cjf@lanl.gov, & Zhang, Hong Lin.
```*Relativistic distorted-wave collision strengths for the 49 Δn=0 optically allowed transitions with n=2 in the 67 B-like ions with 26≤Z≤92*. United States. doi:10.1016/J.ADT.2013.09.001.

```
Fontes, Christopher J., E-mail: cjf@lanl.gov, and Zhang, Hong Lin. Thu .
"Relativistic distorted-wave collision strengths for the 49 Δn=0 optically allowed transitions with n=2 in the 67 B-like ions with 26≤Z≤92". United States. doi:10.1016/J.ADT.2013.09.001.
```

```
@article{osti_22314846,
```

title = {Relativistic distorted-wave collision strengths for the 49 Δn=0 optically allowed transitions with n=2 in the 67 B-like ions with 26≤Z≤92},

author = {Fontes, Christopher J., E-mail: cjf@lanl.gov and Zhang, Hong Lin},

abstractNote = {Relativistic distorted-wave collision strengths have been calculated for the 49 Δn=0 optically allowed transitions with n=2 in the 67 B-like ions with nuclear charge number Z in the range 26≤Z≤92. The calculations were made for the four final, or scattered, electron energies E{sup ′}=0.20, 0.42, 0.80, and 1.40, where E{sup ′} is in units of Z{sub eff}{sup 2} Ry with Z{sub eff}=Z−3.33. In the present 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 and D.H. Sampson, At. Data Nucl. Data Tables 56 (1994) 41]. In that earlier work, collision strengths were also provided for B-like ions, but for a more comprehensive data set consisting of all 105 Δn=0 transitions, six scattered energies and the 85 ions with Z in the range 8≤Z≤92. The collision strengths covered in the present work should be more accurate than the corresponding data given by Zhang and Sampson [H.L. Zhang and D.H. Sampson, At. Data Nucl. Data Tables 56 (1994) 41] and are presented here to replace those earlier results.},

doi = {10.1016/J.ADT.2013.09.001},

journal = {Atomic Data and Nuclear Data Tables},

issn = {0092-640X},

number = 3,

volume = 100,

place = {United States},

year = {2014},

month = {5}

}