Page 99 - Photonics Essentials an introduction with experiments
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Photoconductivity

                                                        Photoconductivity  93

                                                      –3
                                                           –1
          rate of electrons =  f, where  f has units of cm -sec . In the steady
          state, the generation rate and the recombination rate must be the
          same.
            The treatment that follows is based on the description of sensitiza-
          tion given by Rose in  Concepts in Photoconductivity (see Bibliogra-
          phy). In Fig. 5.14, we show an energy level diagram for a typical pho-
          toconductor material such as CdS.
            A recombination level is formed by addition of a single type of impu-
          rity that forms a level near the center of the band gap. The Fermi lev-
          el will fall in the center of these levels, as shown in the figure. Sup-
          pose that the density of the recombination sites is  N. We can now
          define some parameters that we will need for the discussion of sensiti-
          zation:

          1. n r = the density of centers occupied by electrons
          2. p r = the density of centers unoccupied by electrons

            When an electron recombines on an unoccupied site,  p r , the site
          changes to an occupied site and counts as part of n r . At all times, n r +
          p r = N r .
            The chance that an electron recombines on an unoccupied site is
                                                                         2
          measured by the cross-section of the site, s n , which has units of cm .
          The capture cross section for holes by a site occupied by an electron is
          s p . In the steady state:

                                    n = f  n 
 n r
                                                                     (5.15)
                                    p = f  p 
 p r
            A charge carrier moving with a velocity v will travel a distance = v
          on the average before it recombines. The product of the capture cross
          section with this distance gives the effective volume of the recombina-
          tion center, as shown in Fig. 5.15
            The density of unoccupied centers for electrons, p r , is just the in-
          verse of this volume. Thus,
                            1
                              = volume of a center =   n vs n        (5.16)
                           p r
          and
                                             f
                                  n = f  n =                         (5.17)
                                           p r vs n
          To appreciate what these equations mean, we give some typical val-
          ues for these parameters in Table 5.1 for electrons in silicon.
            Since recombination centers promote recombination, their presence
          in general shortens the carrier lifetime. It is always true that increas-

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