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Erratum to “Core level shift in random CuPd and AgPd alloys by the complete screening picture”
Journal of Electron Spectroscopy and Related Phenomena 129 (2003) 81–82 www.elsevier.com / locate / elspec
Erratum
Erratum to ‘‘Core level shift in random CuPd and AgPd alloys by the complete screening picture’’ [J. Electron Spectrosc. Relat. Phenom. 127 (2002) 65–69] q a, a a,b W. Olovsson *, I.A. Abrikosov , B. Johansson a
b
Condensed Matter Theory Group, Department of Physics, Uppsala University, SE-751 21 Uppsala, Sweden Applied Materials Physics, Department of Materials Science and Engineering, Royal Institute of Technology, SE-100 44 Stockholm, Sweden
The publisher regrets that when the above article was published the reference nos. within Figs. 1–4 were incorrect. Figs. 1–4 are reproduced correctly below and on the following page.
Fig. 1. CLS for Cu 2p 3 / 2 in Cu 12x Pd x . The result of the complete screening picture (filled boxes, dashed line) and the initial state approach (empty boxes, dot-dashed line) is compared to two experimental sets (filled and empty circles).
Fig. 2. CLS for Pd 3d 5 / 2 in Cu 12x Pd x . The notation is the same as in Fig. 1.
q
Original PII of article: S0368-2048(02)00173-1 *Corresponding author. E-mail address: [email protected] (W. Olovsson). 0368-2048 / 03 / $ – see front matter 2003 Elsevier Science B.V. All rights reserved. doi:10.1016 / S0368-2048(02)00308-0
82
W. Olovsson et al. / Journal of Electron Spectroscopy and Related Phenomena 129 (2003) 81–82
Fig. 3. CLS for Ag 3d 5 / 2 in Ag 12x Pd x . The complete screening picture (filled boxes, dashed line) and the initial state approach (empty boxes, dot-dashed line) is compared to experimental values ¨ from the work of Steiner and Hufner [16] (empty circles).
Fig. 4. CLS for Pd 3d 5 / 2 in Ag 12x Pd x . The notation is the same as in Fig. 3.
Erratum
Erratum to ‘‘Core level shift in random CuPd and AgPd alloys by the complete screening picture’’ [J. Electron Spectrosc. Relat. Phenom. 127 (2002) 65–69] q a, a a,b W. Olovsson *, I.A. Abrikosov , B. Johansson a
b
Condensed Matter Theory Group, Department of Physics, Uppsala University, SE-751 21 Uppsala, Sweden Applied Materials Physics, Department of Materials Science and Engineering, Royal Institute of Technology, SE-100 44 Stockholm, Sweden
The publisher regrets that when the above article was published the reference nos. within Figs. 1–4 were incorrect. Figs. 1–4 are reproduced correctly below and on the following page.
Fig. 1. CLS for Cu 2p 3 / 2 in Cu 12x Pd x . The result of the complete screening picture (filled boxes, dashed line) and the initial state approach (empty boxes, dot-dashed line) is compared to two experimental sets (filled and empty circles).
Fig. 2. CLS for Pd 3d 5 / 2 in Cu 12x Pd x . The notation is the same as in Fig. 1.
q
Original PII of article: S0368-2048(02)00173-1 *Corresponding author. E-mail address: [email protected] (W. Olovsson). 0368-2048 / 03 / $ – see front matter 2003 Elsevier Science B.V. All rights reserved. doi:10.1016 / S0368-2048(02)00308-0
82
W. Olovsson et al. / Journal of Electron Spectroscopy and Related Phenomena 129 (2003) 81–82
Fig. 3. CLS for Ag 3d 5 / 2 in Ag 12x Pd x . The complete screening picture (filled boxes, dashed line) and the initial state approach (empty boxes, dot-dashed line) is compared to experimental values ¨ from the work of Steiner and Hufner [16] (empty circles).
Fig. 4. CLS for Pd 3d 5 / 2 in Ag 12x Pd x . The notation is the same as in Fig. 3.