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 Encyclopedia of Physical Science and Technology  en001f-44  May 7, 2001  15:8






               788                                                                             Auger Electron Spectroscopy


               bibliography will provide the interested reader with a start
               in this field.
                 An obvious question that must be answered is why
               Auger electron spectroscopy has achieved this place in
               the surface analytical field. First of all, it is a relatively
               straightforward technique to use, and high-quality com-
               mercial spectrometers are available. The data are easily
               interpretable, at least on a qualitative level, and it is also
               possible to use an incident beam that is well under 1 µm
               in diameter. This diameter is several orders of magnitude
               smaller than what is possible for most other surface an-
               alytical techniques, and this fact means that Auger spec-
               troscopy can be used to probe changes in composition
               across a surface at a microscopic scale. Finally, Auger
               electron spectroscopy can detect every element except hy-  FIGURE 1 Energy level diagram representing de-excitations by
                                                                 (a) Auger electron emissions and (b) X-ray fluorescence. In the
               drogen and helium, so it useful for studying both light and
                                                                 particular Auger process that is shown, a K-shell hole is first cre-
               heavy element. We now wish to consider Auger electron  ated and an electron in the L I shell drops down to fill it. In so doing,
               spectroscopy and the process on which it is based.  it gives off enough energy to knock an electron out of the L III shell,
                                                                 which becomes the Auger electron.
               II. THE AUGER PROCESS AND AUGER
                  ELECTRON SPECTROSCOPY                          solid must come from very near the surface of the solid.
                                                                 Although the yield of Auger electrons will again depend
               When an electron beam impinges on a solid surface, it can  on the particular element, it is estimated that most come
               knock out inner shell electrons if it is of sufficient energy.  from the top two to five atom layers.
               The holes that are left behind will then be filled by having  It had been recognized for some years after their discov-
               outershellelectronsfallintothem.Thislastprocessoccurs  ery that Auger electrons might provide a chemical analysis
               with the emission of energy, since the outer shell electron  of a surface, but it was not until the work of L. A. Harris
               is changing from a higher to a lower energy. The energy  in 1968 that the technique actually became feasible in the
               that is given off can cause one of two events to occur. The  laboratory. Prior to Harris’ work, the problem had always
               energy can simply escape from the solid as an X-ray; in  been that the Auger signal was so small compared with
               this case, the process of X-ray fluorescence has occurred.  that from other types of emitted electrons that it could not
               In the other case, this energy can knock out another outer  be adequately detected. Harris applied a phase-sensitive
               shell electron. These electrons are the Auger electrons that  detection scheme in which a small, regularly oscillating
               were named for Pierre Auger who discovered this process  voltage was superimposed on a larger, constantly increas-
               in 1929. Such processes are usually denoted by the shells  ing voltage. By measuring the electrons being collected,
               of the electrons that are involved. Thus, a KLL Auger  he was able to detect a small perturbation in the number
               process means that the first electron that was knocked out  of electrons at a given energy level, because the increased
               was from the K shell, the hole was filled by an electron  yield would be in phase with the frequency of the oscillat-
               from an L shell, and the Auger or secondary electron that  ing voltage. By electronically differentiating the signal in
               was emitted was also from an L shell.             this way, he could help bring out these small peaks. With
                 Figure 1 shows the processes of Auger emission and flu-  this advance, the use of Auger electrons to measure sur-
               orescence schematically. The frequency with which one  face composition became a reality. Today, one can simply
               of them will occur relative to the other depends on the  obtain differentiated spectra such as those shown in Fig. 2
               particular element; but as a rule of thumb, it can be re-  and identify the elements present on the surface by com-
               membered that elements with low atomic numbers tend to  paring the energies of the peaks with those in handbooks
               favor the Auger process, whereas those with high atomic  of elemental standards.
               numbers favor fluorescence. The Auger electrons that are  Although Harris’ contribution was pivotal in the devel-
               emitted have energies that are characteristic of the element  opment of Auger electron spectroscopy, there have been
               from which they came. Therefore, if they can be detected  other advances since his that have helped Auger electron
               they will provide a method of chemical analysis. Further-  spectroscopy to become such a useful surface analytical
               more, since the electrons that arise from such a process are  technique. One of the most important was the development
               going to be of low energy, those that do escape from the  of the cylindrical mirror analyzer by Palmberg, Bohn, and
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