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340                           Optoelectronics

                                     In a phototransistor the base is not connected. Instead, it is exposed to the
                                   input light, which creates the carriers providing the base current. The base
                                   current is then amplified in the usual manner.
                                     Perhaps I should add that amplification is a good thing but not the only
                                   thing to consider. Under certain conditions noise performance may be a more
                                   important criterion when choosing a particular detector.
                                     All the photodetectors mentioned so far needed an applied voltage. It should
                                   be noted, however, that it is not necessary in this case. Light may be detected
                                   in a p–n junction simply by short-circuiting it via a microammeter of very
                                   low resistance, which serves as the load. The electrons and holes generated
                                   by light in the junction will move under the effect of the built-in voltage and
                                   drive a current through the ammeter. The measured current turns out to be
                                   proportional to the input light intensity. This arrangement is usually referred
                                   to as the photovoltaic operation of the junction.
                                     A photovoltaic cell energized by the sun becomes a solar battery. When we
                                   used to worry about the ‘energy crisis’ it was hoped that acres of solar cells
                                   would replace nasty, dirty power stations. This has not quite come off, mainly
                                   for economic reasons. A simple calculation shows that, even with a generous
                                   estimate for the lifetime of a solar cell, the total energy it will generate is less
                                   than that required to purify and fabricate the single crystal slice from which
                                   it is made. So single crystals are definitely out, except for applications when
                                   money is no object—as in space vehicles. Amorphous materials, however,
                                   which we briefly discussed in Section 8.9, can be used, as the economics
                                   are more favourable. The amorphous semiconductor with the most advanced
                                   technology is silicon. It is possible to process it in a wide variety of ways,
                                   so that its texture absorbs light well, and the actual absorption edge can be
                                   shifted to give a better match to the sun’s output than is obtained by the much
                                   more clearly defined single crystal. Amorphous silicon is usually deposited
                                   in a vacuum or reduced gas pressure as a thin film. This makes it possible to
                                   optimize the film thickness—thick enough to absorb light, but not so massive
               First junction      that the much shorter carrier lifetimes and diffusion lengths lead to loss of
                 GaInP
               absorbs light       carriers before they participate in useful current. A typical solar cell would
               E > 1.85 eV         consist of successive n- and p-layers sputtered on a metallized substrate and
              tunnel junction
              second junction      superposed by a transparent metal top electrode. There are many varieties and,
                 GaAs              in fact, the variables are so numerous that solar cells have made many PhD
               absorbs light
             1.85eV > E > 1.4eV    theses but have not yet solved the energy problem. However, one commercial
              tunnel junction      realization, now commonplace, is the solar battery driven calculator.
              third junction         Other materials that have seemed promising include CdTe and CuInSe 2
                GaInAs
               absorbs light       as components in multistage solar converters which absorb some of the light
              1.4eV > E > 1eV      photovoltaically and reflect or transmit other wavelengths to different energy
              tunnel junction      gap devices.
              fourth junction
                  Ge                 One advantage of working as a photovoltaic engineer is that you have two
               absorbs light       levels of costing and seeking efficiency. On the one hand, there is the space
             1eV > E > 0.67eV
                                   vehicle market where photovoltaics are looked upon as essential but relat-
               GaAs or Ge
                substrate          ively cheap accessories to a vehicle whose cost is astronomical, so a bit more
                                   efficiency is worth paying for. On the other hand there is the power station re-
     Fig. 13.3                     placement market where you need acres of photo cells and your competitor is
     Schematic drawing of proposed  coal which comes out of the ground with low cost.
     four-junction solar cell, parts of  Figure 13.3 is a schematic drawing of a four-level solar cell. It uses a thin
     which have been made and tested.
                                   top layer of GaInP with an energy gap of 1.85 eV, then successive layers of
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