Page 266 - Phase-Locked Loops Design, Simulation, and Applications
P. 266

MIXED-SIGNAL PLL APPLICATIONS PART 1: INTEGER-N FREQUENCY
             SYNTHESIZERS   Ronald E. Best                                                          157
             with  U  = amplitude of the fundamental of the VCO output  signal. After a number of
                    0
             trigonometric manipulations, we finally get



                                                                                                      (6.45)


               Apparently u (t) consists of a carrier at radian frequency ω , plus two side-bands displaced
                            2                                           0
             by  ±  f  from the carrier. We can therefore calculate the carrier to sideband ratio  S  at
                                                                                                    1
                    ref
             frequency offset f  from
                             ref






               Using the relations


                                                                                         [cf.      Eq.
                                                                                      (2.27)]



                                                                                         (cf.      Fig.
                                                                                      2.17b)


                                                                                         [cf.      Eq.
                                                                                      (3.23)]



                                                                                         [cf.      Eq.
                                                                                      (3.23)]

             we finally get



                                                                                         (6.46)


               We recognize that the carrier-to-spur ratio decreases with the square of the current
             imbalance δ.
               We conclude this chapter with a note regarding suppression of spurs by the loop filter. As
             we know, spurs mostly occur at the reference frequency and multiples thereof. They are easily
             suppressed when the loop bandwidth (f    ) is chosen to be less than the reference frequency.
                                                   3dB
             Second-order PLLs, as they were analyzed in Chap. 3, show a relatively flat gain rolloff at
             higher frequencies, because  the phase-transfer function  H(s) has two poles and one zero.
             Consequently, the gain rolls off with only −20 dB/decade at higher frequencies. The spurs are
             therefore only partially suppressed. A better spur suppression is obtained when higher-order
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