Page 18 - Complete Wireless Design
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Wireless Essentials



                                                                              Wireless Essentials  17


















                         Figure 1.20 PIN diode forward-bias current and RF resistance.


                          Zero-bias Schottkys are a type of diode with a very low forward voltage.
                        Figure 1.21 displays their I-V curves, showing their low forward voltage and
                        the resultant forward current.

                        Gunn diodes. Gunn diodes can function as an oscillator at microwave fre-
                        quencies. The transit time of an electron through the Gunn diode determines
                        the actual frequency of oscillation and, when the diode is inserted into a suit-
                        able resonant cavity, the Gunn device can oscillate at frequencies of up to 100
                        GHz. However, the higher the frequency of the Gunn, the thinner it must be,
                        which lowers its power dissipation abilities.

                        Step-recovery diodes. A step-recovery diode (SRD) is a special diode employed
                        in some microwave frequency-multiplication circuits. The SRD functions in
                        this role by switching between two impedance conditions: low and high. This
                        change of state may occur in only 200 ps or less, thus discharging a very nar-
                        row pulse of energy. An SRD can best be visualized as a capacitor that stores
                        a charge, then discharges it at a very rapid rate, causing a pulse that is plen-
                        tiful in harmonics.


            1.2.3 Transistors

                        Bipolar junction transistor (BJT). A bipolar transistor is constructed of NPN or
                        PNP doped regions, with the NPN being by far the most common. The emitter
                        provides the charges, while the base controls these charges. The charges that
                        have not entered the base are gathered by the collector.
                          Figure 1.22 reveals a silicon NPN transistor that has its emitter and base
                        forward biased, with the collector reversed biased, to form a simple amplifier.
                        The negative terminal of the emitter-base battery repels the emitter’s elec-
                        trons, forcing them into the thin base. But the thin base structure, because of
                        the small amount of holes available for recombination, cannot support the
                        large number of electrons coming from the emitter. This is why base current


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