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Mixed-Signal (SOP) Design   187



                            Component                 Value                     Q
                                L 1                  12.5 nH               60 @ 0.9 GHz
                                L                      8 nH                57 @ 0.9 GHz
                                2
                                L                      7 nH                62 @ 0.9 GHz
                                 i
                               C 1                   0.22 pF               260 @ 1.8 GHz
                               C 2                     2 pF                247 @ 1.8 GHz
                                C                      2 pF                253 @ 1.8 GHz
                                 i
                    TABLE 4.5  Component Parameters for Oscillator



                    In Equation (4.11) S is the reflection coefficient corresponding to the input impedance
                                     in
                    Z  and Γ  is the reflection coefficient of the input resonator. The basic idea is to generate
                     in
                            r
                    instability at two frequencies so that the oscillator circuitry can be adjusted to satisfy
                    Equation (4.11) at the two frequencies. Circuit simulations show that an inductance of
                    29 nH at 900 MHz and an inductance of 19 nH at 1.8 GHz is required at the base terminal
                    to generate instability at 900 MHz and 1.8 GHz, respectively. For sustained oscillations
                    the load at the collector should also be frequency dependent [46]. Hence, a dual-band
                    Chebychev bandpass filter is used as the matching network at the collector, as shown in
                    Figure 4.35. The filters are designed to match the core of the oscillator at their designed
                    center frequency while providing very low insertion loss (∼1.5 dB). The input resonator
                    is designed to provide capacitive reactance at 900 MHz and inductive reactance at
                    1.8 GHz. The reactance of the input resonator cancels the reactance observed at the
                    emitter terminal thereby satisfying the oscillation conditions in Equation (4.11).
                       Prior to design, it is important to estimate the component values required and their
                    corresponding unloaded quality factors that provide the necessary performance. This
                    can be evaluated using any RF circuit simulator such as Advanced Design System
                    (ADS) from Agilent Technologies or Spectre from Cadence. The results are tabulated in
                    Table 4.5, for the VCO, and Table 4.6 shows the component values used in the design of
                    the Chebychev filter.




                            Component                 Value                     Q
                          C , C , C , C 44            0.6 pF               260 @ 0.9 GHz
                                  33
                               22
                           11
                               C                      0.18 pF              269 @ 0.9 GHz
                                c1
                               C                      0.23 pF              262 @ 0.9 GHz
                                c2
                               C s1                   1.5 pF               245 @ 0.9 GHz
                               C s2                    1 pF                247 @ 1.8 GHz
                                L a                   13 nH                59 @ 0.9 GHz
                                L                     4.2 nH               79 @ 1.8 GHz
                                 b
                    TABLE 4.6  Component Parameters for Chebyshev Filters
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