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172                                                    C. AMOVILLI AND R. McWEENY













































                         KL-LLL  (‘monopole ionizations’);  and  KLe–LL or Ke–L  (‘high-energy satellites’).
                         From Table 5 it is possible to estimate the energies of transition for various pairs of
                         states, even though the  ‘state’ energies are stricly speaking configurational averages.
                         Figure 1  shows  (vertical lines)  the estimated values of these transition energies, su-
                         perimposed on  the experimental spectrum. It is noteworthy that,  even if the vertical
                         lines are not actually coincident with the peak positions, the assignment of the peaks
                         for various processes is  substantially in accord with that  made by Moddeman et  al
                         [21] on the basis of the experimental data.
                         References

                            1. L. Brillouin, Actualités Sci.  et Ind., No.  71, (1933).
                            2. L. Brillouin, Actualités Sci.  et Ind., No.  159, (1934).
                           3.  T. A. Koopmans, Physica 1, 104, (1933).
                           4. G. Berthier, in Current Aspects of Quantum Chemistry, R. Carbó (Ed.), Else-
                              vier, Amsterdam, 1982, pp. 145-156.
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