Page 222 - Phase-Locked Loops Design, Simulation, and Applications
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MIXED-SIGNAL PLL APPLICATIONS PART 1: INTEGER-N FREQUENCY
             SYNTHESIZERS   Ronald E. Best                                                          135
             fed to a mixer that creates the IF signal. Now assume that an interfering signal is present at
             frequency f , which is not far away from f , may be at a distance of only 200 kHz from f .
                                                       d,
                                                                                                      d
                        int
             This could be another communication signal that has perhaps a much greater amplitude than
             the desired signal. If the spectrum of the LO at frequency  f  +  f  shows appreciable
                                                                            int
                                                                                  IF
             amplitude (as shown by line A  in the figure), the interferer is also mixed down to the
             intermediate frequency. This phenomenon is called reciprocal mixing. When the interfering
             signal is 100 dB greater than that desired and the noise spectrum of the LO is “only” 100
             dB below its carrier amplitude, these two signals produce the same mixer output power. In
             many mobile communications, the individual channels are  spaced by 200 kHz. To avoid
             reciprocal mixing by an interferer whose frequency is immediately adjacent to the desired
             channel frequency, the noise spectrum of the LO must be markedly more than 100 dB below
             the carrier amplitude at a distance of 200 kHz from that carrier.  Frequency synthesizers
             intended for such applications impose, therefore, very tight requirements on phase noise and
             spurs. It should be noted that in many applications the IF frequency f  is chosen 0 (zero IF
                                                                                 IF
             systems).
               In the following, we will investigate the sources of those undesired noise components. The
             mathematical analysis is quite cumbersome,  but fortunately there are a number of models
             available that greatly simplify the analysis. Basically, each part of the synthesizer circuit can
                                           48
             contribute to output phase jitter.  In the following, we will concentrate on the dominant ones.
             Figure 6.14 shows a simplified model for the determination of output phase noise and spurious
             sidebands.
               Three sources of phase jitter and spurs can be recognized:

             ■ Phase jitter is created by the reference oscillator. Even the highest quality reference
               oscillator is not free from output phase jitter. This perturbation is denoted as θ n,ref .
             ■ Phase jitter created by the VCO. Because the VCO is nothing else than an oscillator, it also
               will contribute to phase jitter. This perturbation is denoted as θ n,VCO .
























                      Figure 6.14 A model for analysis of output phase jitter θ n,out  in a PLL frequency synthesizer.
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