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The Electronic System
                             repulsion and quantum mechanical attraction has a minimum for a finite
                              . b
                             3.3.3 Types of Band Structures

                Valence and   The graphical solution of (3.97) as given in Figure 3.11 provides us with
                Conduction   the possible electronic states that can be occupied by electrons. In a semi-
                Bands
                             conductor the Fermi energy lies in the gap between two bands, i.e., there
                             is an uppermost completely filled band called the valence band. The fol-
                             lowing unoccupied band is called the conduction band. As we shall see in
                             Section 5.4, this band contains a certain number of electrons depending
                             on the temperature of the electronic system.


                                           k
                Si, Ge, GaAs  The wave-vector   entering the r.h.s. of (3.97) so far was taken in its lim-
                                                       ⁄
                             iting cases  k =  0   and  k =  π L  , resulting in the upper and lower
                             bounds of the bands by the fact that  cos 0 =  1   and  cos π =  – 1  . We
                             know ask for the structure of the bands in between those two limits for
                                         ,
                                            ⁄
                             arbitrary k ∈  [ 0 π L]  . From Section 2.2 we know that this corresponds
                             to the center and the edge of the Brillouin zone. The crystal structure is
                             not isotropic and therefore we shall have different band structures in the
                             respective crystal directions. This leaves us with a function E k()  , where
                                                                              i
                             i is the band index in Figure 3.11 and   is now a real three-dimensional
                                                            k
                             vector. In Figure 3.13 the typical band structure for cubic crystals is
                             shown in different crystallographic directions. There are several things to
                             observe in Figure 3.13:

                             • after passing the edge of the Brillouin zone they periodically repeat;
                             • the valence band, i.e., the uppermost occupied band is separated by an
                               energy gap E   from the conduction band (the valence bands are high-
                                          g
                               lighted);
                             • in general, the minimum energy of the conduction band is not neces-
                               sarily found at the same k-value as the maximum of the valence band
                               (points B or D are lower in energy than point C). This is called an
                               indirect band gap as is the case for Si and Ge. GaAs shows a direct


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