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/content/aip/journal/jcp/87/5/10.1063/1.453017
1.
1.A. P. Hitchcock and J. Stöhr, J. Chem. Phys. 87, 3253 (1987).
2.
2.M. N. Piancastelli, D. W. Lindle, T. A. Ferrett, and D. A. Shirley, J. Chem. Phys. 86, 2765 (1987).
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3.J. L. Dehmer, D. Dill, and S. Wallace, Phys. Rev. Lett. 43, 1005 (1979).
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4.J. R. Swanson, D. Dill, and J. L. Dehmer, Phys. Rev. B 14, L207 (1981).
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5.M. N. Piancastelli, P. R. Keller, J. W. Taylor, F. A. Grimm, T. A. Carlson, M. O. Krause, and D. Lichtenberger, J. Electron Spectrosc. Relat. Phenom. 34, 205 (1984).
6.
6.F. Sette, J. Stöhr, and A. P. Hitchcock, J. Chem. Phys. 81, 4906 (1984).
7.
7.One other possible “process” omitted from the discussion in Ref. 2 is that maxima in absorption may be due to the accidental sum of several different and distinct continuum eigenchannels, and thus not resonances at all.
8.
8.H. P. Hitchcock, S. Beaulieu, T. Steel, J. Stöhr, and F. Sette, J. Chem. Phys. 80, 3927 (1984).
9.
9.By proof, it does not suffice to symmetry label an absorption feature as σ or π by virtue of polarization‐dependent studies, because other processes, such as double excitation, may show the same symmetry as a supposed shape resonance.
10.
10.C. M. Truesdale, D. W. Lindle, P. H. Kobrin, U. E. Becker, H. G. Kerkhoff, P. A. Heimann, T. A. Ferrett, and D. A. Shirley, J. Chem. Phys. 80, 2319 (1984).
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/content/aip/journal/jcp/87/5/10.1063/1.453017
1987-09-01
2016-12-03
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