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1
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N. Wassdahl, A. Nilsson, T. Wiell, H. Tillborg, L.C. Duda, J.H. Guo, N. Mårtensson, J. Nordgren, J.N. Andersen and R. Nyholm, Phys. Rev. Lett. 69 (1994) 812.
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Phys. Rev. Lett.
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Wassdahl, N.1
Nilsson, A.2
Wiell, T.3
Tillborg, H.4
Duda, L.C.5
Guo, J.H.6
Mårtensson, N.7
Nordgren, J.8
Andersen, J.N.9
Nyholm, R.10
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2
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0028385315
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T. Wiell, H. Tillborg, A. Nilsson, N. Wassdahl, N. Martensson and J. Nordgren, Surf. Sci. 304 (1994) L451.
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Surf. Sci.
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Wassdahl, N.4
Martensson, N.5
Nordgren, J.6
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3
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0000858531
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(a) A. Nilsson, P. Bennich, T. Wiell, N. Wassdahl, N. Mårtensson, J. Nordgren, O. Björneholm and J. Stöhr, Phys. Rev. B 51 (1995) 10244;
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Phys. Rev. B
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Nilsson, A.1
Bennich, P.2
Wiell, T.3
Wassdahl, N.4
Mårtensson, N.5
Nordgren, J.6
Björneholm, O.7
Stöhr, J.8
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4
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0043215630
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to be published
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(b) P. Bennich, A. Nilsson, T. Wiell, N. Wasdahl, N. Mårtensson, J. Nordgren, O. Björneholm, J. Stöhr, J. Bustad and S. Lunell, to be published.
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Bennich, P.1
Nilsson, A.2
Wiell, T.3
Wasdahl, N.4
Mårtensson, N.5
Nordgren, J.6
Björneholm, O.7
Stöhr, J.8
Bustad, J.9
Lunell, S.10
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14
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0002000577
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Eds. J. Labanowski and J. Andzelm Springer, New York
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D.R. Salahub, R. Fournier, P. Mlynarski, I. Papai, A. St-Amant and J. Ushio, in: Density Functional Methods in Chemistry, Eds. J. Labanowski and J. Andzelm (Springer, New York, 1991) p. 77; A. St-Amant, Ph.D. Thesis, Université de Montréal, 1992. The present version of the program has been substantially modified by L.G.M. Pettersson.
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(1991)
Density Functional Methods in Chemistry
, pp. 77
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Salahub, D.R.1
Fournier, R.2
Mlynarski, P.3
Papai, I.4
St-Amant, A.5
Ushio, J.6
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15
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0042714465
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Ph.D. Thesis, Université de Montréal
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D.R. Salahub, R. Fournier, P. Mlynarski, I. Papai, A. St-Amant and J. Ushio, in: Density Functional Methods in Chemistry, Eds. J. Labanowski and J. Andzelm (Springer, New York, 1991) p. 77; A. St-Amant, Ph.D. Thesis, Université de Montréal, 1992. The present version of the program has been substantially modified by L.G.M. Pettersson.
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(1992)
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St-Amant, A.1
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16
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0000682298
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A. Mattsson, I. Panas, P. Siegbahn, U. Wahlgren and H. Åkeby, Phys. Rev. B 36 (1987) 7389.
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Phys. Rev. B
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Mattsson, A.1
Panas, I.2
Siegbahn, P.3
Wahlgren, U.4
Åkeby, H.5
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17
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0003699557
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Ed. D. Salahub Kluwer, Dordrecht
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U. Wahlgren and P.E.M. Siegbahn, in: Metal-Ligand Interactions: from Atoms, to Clusters, to Surfaces, Ed. D. Salahub (Kluwer, Dordrecht, 1991).
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Metal-ligand Interactions: From Atoms, to Clusters, to Surfaces
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Wahlgren, U.1
Siegbahn, P.E.M.2
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22
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0042213351
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note
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The ECP modifications for DISCO were written by L.G.M. Pettersson.
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27
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0042213350
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note
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The population analysis is better defined for small basis sets, and the one-center model is strictly defined only for single zeta basis sets [4]. Since the total intensity at the DZ level represents the large basis set spectra quite well, one-center spectra based on population analysis with the DZ-basis sets should be the most appropriate.
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28
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0001381715
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H. Antonsson, A. Nilsson, N. Mårtenson, I. Panas and P.E.M. Siegbahn, J. Electron Spectrosc. Relat Phenom. 54/55 (1990) 601.
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(1990)
J. Electron Spectrosc. Relat Phenom.
, vol.54-55
, pp. 601
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Antonsson, H.1
Nilsson, A.2
Mårtenson, N.3
Panas, I.4
Siegbahn, P.E.M.5
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29
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0001599682
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W. Wurth, C. Schneider, R. Treichler, E. Umbach and D. Menzel, Phys. Rev. B 35 (1987) 7741.
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(1987)
Phys. Rev. B
, vol.35
, pp. 7741
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Wurth, W.1
Schneider, C.2
Treichler, R.3
Umbach, E.4
Menzel, D.5
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30
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0001484796
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A. Sandell, O. Björneholm, A. Nilsson, B. Hernäs, J.N. Andersen and N. Mårtensson, Phys. Rev. B 49 (1994) 10136.
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(1994)
Phys. Rev. B
, vol.49
, pp. 10136
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Sandell, A.1
Björneholm, O.2
Nilsson, A.3
Hernäs, B.4
Andersen, J.N.5
Mårtensson, N.6
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31
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0043215628
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private communication
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J. Nordgren, private communication.
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Nordgren, J.1
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32
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0041712920
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D. Menzel, P. Feulner, R. Treichler, E. Umbach and W. Wurth, Phys. Scr. 17 (1986) 166.
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(1986)
Phys. Scr.
, vol.17
, pp. 166
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Menzel, D.1
Feulner, P.2
Treichler, R.3
Umbach, E.4
Wurth, W.5
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34
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0041712922
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note
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The large intensity of the n * elastic peak is due to the unusual role of screening in the carbon spectrum, unaccounted for by the final state frozen anion. Separate state MCSCF optimizations [33] predict a factor of 3 for the relative π * and 5σ intensities, in good accordance with the experimental resonant X-ray emission spectrum [29].
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