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Chapter 2 The Crystal
                                              Lattice System























                            In this chapter we start our study of the semiconductor system with the
                                           (
                            crystals of silicon  Si)  , adding some detail on crystalline silicon dioxide
                             ( SiO )   and to a lesser extent on gallium arsenide  GaAs)  . All three are
                                                                     (
                                 2
                            regular lattice-arrangements of atoms or atoms. For the semiconductors
                            silicon and gallium arsenide, we will consider a model that completely
                            de-couple the behavior of the atoms from the valence electrons, assuming
                            that electronic dynamics can be considered as a perturbation to the lattice
                            dynamics, a topic dealt with in Chapter 3. For all the electrons of the
                            ionic crystal silicon dioxide, as well as the bound electrons of the semi-
                            conductors, we here assume that they obediently follow the motion of the
                            atoms.

                            We  will see that by applying the methods of classical, statistical and
                            quantum mechanics to the lattice, we are able to predict a number of
                            observable constitutive phenomena of interest—i.e., we are able to
                            explain macroscopic measurements in terms of microscopic crystal lat-
                            tice mechanics. The effects include an approximation for the elastic coef-


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