Page 208 - Electrical Properties of Materials
P. 208

190                           Principles of semiconductor devices

                                                         +   –
                                                                         Depletion
                                                                          regions
                                      Signal                     Gate             n-type
                                      input  ~                                    semiconductor
                                                                            Drain
                                        Source
                                                                                        I DS
                                                                              +
                                                                             n  - contact
     Fig. 9.32
     Schematic representation of a                               Gate                    Signal
     field-effect transistor (FET). The                                                   output
                                                                                    R
     current between source and drain is                  p  - material              L
                                                           +
     controlled by the voltage on the gate         –   +
     electrodes.
                                   and both make use of electrons and holes. They work, though, on entirely dif-
                                   ferent principles. The basic idea of the FET originated in the 1920s, although
                                   any practical realization had to wait until the 1950s. It consists of a piece of
                                   semiconductor—let us suppose n-type—to which two ohmic contacts, called
                                   the source and the drain, are made (Fig. 9.32). As may be seen, the drain is pos-
                                   itive: thus electrons flow from source to drain. There is also a gate electrode
                                                                                +
                                   consisting of a heavily doped p-type region (denoted by p ). Let us assume for
                                   the time being that U SG , the voltage between source and gate, is zero. What
                                   will be the potential at some point in the n-type material? Since there is an
                                   ordinary ohmic potential drop due to the flow of current, the potential grows
                                                                                               +
                                   from zero at the earthed source terminal to U DS at the drain. Hence, the p n
                                   junction is always reverse biased with the reverse bias increasing towards the
                                   drain. As a consequence, the depletion region has an asymmetrical shape as
                                   shown in Fig. 9.32. The drain current must flow in the channel between the
                                   depletion regions.
                                     If we make the gate negative, then the reverse bias, and with it the depletion
                                   region, increases, forcing the current to flow through a narrower region, that is
                                   through a higher resistance. Consequently, the current decreases. Making the
                                   gate more and more negative with respect to the source, there will obviously
                                   be a voltage at which the depletion regions join and the drain current decreases
                                   to practically zero as shown in Fig. 9.33(a). This I D versus U GS characteristic



                                       (a)                 (b)
                                                     I         I
                                                     D         D
                                                                             U  = 0
                                                                              GS
                                                                                   U  decreasing
                                                                                    GS





     Fig. 9.33
     The characteristics of a junction type          0      0
                                      U                                               U
     field-effect transistor.           GS                                               DS
   203   204   205   206   207   208   209   210   211   212   213