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               86                                                                               Photoelectron Spectroscopy


               negative relaxation shifts. As suggested in Section II.B,
               the final state relaxation is largest for the molecules that
               contain easily polarizable substituents. In Fig. 27, the  ε
               values obtained from the experimental binding energy
               shifts and the experimentally estimated relaxation contri-
               bution are compared to the charge at the phosphorus atom
               and the off-atom potential, both calculated by a semiem-
               pirical quantum chemical method. The excellent correla-
               tion obtained for this example tells us that the theoretical
               method used is suitable for predicting reasonable atomic
               charges.
                 The energies shown in Table VII were obtained from
               gaseous samples. For solids, an additional problem arises
               that is connected with the reference problem (Section I.E).
               For solids, the binding energies are usually referred to the
               Fermi level and not to the vacuum level. The binding en-
               ergy shifts which appear in Eq. (12), however, refer to the
               vacuum level. Binding energy shifts referred to the Fermi
               level and those referred to the vacuum level are equal only
               when the work function is the same for both samples. If
               this is not the case, the work function difference, which
               in principle is also an experimentally obtainable quantity,
               must be taken into consideration.


               D. Investigation of Adsorbates
               When a molecule is adsorbed at the surface of a solid it
                                                                 FIGURE 28 Comparison of C 1s and O 1s spectra for free
               can be either physisorbed or chemisorbed. We speak of  CO, W(CO) 6 , and CO adsorbed on W(110) and Cu(100). [From
               “physisorption” when the bonding is mainly caused by  Freund, H. J., and Plummer, E. W. (1981). Phys. Rev. B 23, 4859.]
               van der Waals interactions and of “chemisorption” when
               we have some type of a chemical bond between adsorbate
               and substrate. However, there is a more or less continuous  contribute strongly to the understanding of the chemisorp-
               transition between both types of bonding. The nature of  tion bond. Figure 28 shows an example. The C 1s and O
               the bonding between adsorbate and substrate is very im-  1s spectra of gaseous CO are shown at the bottom. Weak
               portant for the understanding of reactions that take place  satellite structures at the high binding energy side of the
               in heterogeneous catalysis. Catalytic processes of this type  main lines are blown up in the figure in order to reveal
               have great technical importance but often they are not fully  their structure. The indicated satellites are connected with
               understood on a molecular level. Because of its extreme  final ion states in which, in addition to the removal of a
               surface sensitivity, PES is a powerful tool in achieving  core electron, a second electron is excited from the π to
                                                                      ∗
               such an understanding. The applications of PES to the  the π orbital. When CO is adsorbed on the 110 surface
               study of adsorbates are too widespread to be reviewed  of tungsten, a new satellite is observed closer to the main
               here. We only show two examples to give an impression  line. This new satellite increases strongly in intensity with
               of how these studies can be carried out.          decreasing strength of the chemisorption bond. For the
                 Foravarietyofadsorbatesystemssuchastheadsorption  system CO on copper (100) (at the top in Fig. 28), where
               of small molecules (CO, N 2 ,H 2 O, etc.) on transition metal  CO is only weakly bound, this new satellite becomes very
               surfaces, a “molecular view” of the bonding often provides  strong. What is the nature of this satellite and what does
               a useful description. In a molecular view we do not look  it tell us about bonding? The fact that the same satellite as
               at the substrate as a metal with band structure and all the  observed for CO on W(110) is also observed in the metal
               typical solid-state properties. Instead, we look primarily  complex W(CO) 6 reveals that this satellite cannot result
               at a few metal atoms to which the adsorbed molecule is  from the special properties of metallic tungsten. It must
               bound. Such a view immediately connects the bonding in  be related to the local bonding between CO and a tungsten
               an adsorbate to the bonding in a metal complex. Thus,  atom. The satellite is connected with a final state where, in
               studying adsorbates together with related complexes can  addition to the core ionization, an electron is transferred
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