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MPhil thesis of Lo Chi Wa - Department of Electronic & Computer ...

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conductance (Gm) and the reciprocal <strong>of</strong> the resistance (1/R) if the amplitude <strong>of</strong>oscillation is not too large. If the amplitude <strong>of</strong> oscillation is larger, the excess noisefactor will be even larger.gdoGmVinFig. 29 gdo for different negative conductancesSince the oscillation amplitude only depends on the tail current <strong>of</strong> the negative Gm celland the parallel equivalent resistance, by designing a Gm cell with the smallest peakGm will give the best phase noise performance. The Gm should be always a bit largerthan 1/R within the oscillation range. This can be done by using the transistors with asmall W/L ratio to implement the negative Gm cell. However, since the negative Gm isjust a bit larger than the 1/R. When the loss <strong>of</strong> the LC tanks is larger due to incorrectmodeling <strong>of</strong> the inductor or varactor, the oscillator cannot oscillate. For example, asshown in Fig. 30, for an oscillator with optimal W/L transistors, if the loss is double,then four times <strong>of</strong> the original current is needed to compensate the loss. It is because thepeak tranconductance <strong>of</strong> the transistor is proportional to the square root <strong>of</strong> the current.As a result, at least four times <strong>of</strong> the original current is required for the doublecompensation and provide an unexpected double amplitude. However, if the designednegative conductance has a larger peak value, only double <strong>of</strong> current are need to43

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