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Radio Frequency Integrated Circuit Design - Webs

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182 <strong>Radio</strong> <strong>Frequency</strong> <strong>Integrated</strong> <strong>Circuit</strong> <strong>Design</strong><br />

Also, it should be noted that this relationship only holds true if the transistor<br />

does not start to saturate. If it does, the nonlinearity will get much worse.<br />

6.4.3 High-<strong>Frequency</strong> Nonlinearity in the Bipolar Transistor<br />

Many frequency-dependent devices can reduce the linearity of a circuit. One<br />

of the most troublesome is the base-collector junction capacitance C� . This<br />

capacitance is voltage dependent, which results in a nonlinearity. This nonlinearity<br />

is especially important in circuits with low supply voltages because the<br />

capacitance is largest at low reverse bias.<br />

This capacitor’s effect is particularly harmful for both frequency response<br />

and nonlinearity in the case of a standard common-emitter amplifier. In this<br />

configuration, C� is multiplied by the gain of the amplifier (the Miller effect)<br />

and appears across the source.<br />

The value of C� as a function of bias voltage is given by<br />

C� (V ) =<br />

C�o<br />

�1 − V<br />

� o� (1/n)<br />

(6.94)<br />

where C�o is the capacitance of the junction under zero bias, � o is the builtin<br />

potential of the junction, and n is usually between 2 and 5. Since this<br />

capacitor’s behavior is highly process dependent and hard to model, there is<br />

little benefit in deriving detailed equations for it. Rather, the designer must rely<br />

on simulation and detailed models to predict its behavior accurately.<br />

6.4.4 Linearity in Common-Collector Configuration<br />

The common-collector amplifier is often called the emitter-follower because the<br />

emitter voltage ‘‘follows’’ the base voltage. However, the amplifier cannot do<br />

this over all conditions. If the current is constant, vBE is constant and the<br />

transfer function will be perfectly linear. However, as vo changes, and iout =<br />

vo /R out will change as shown in Figure 6.31. Thus, iE will change and so will<br />

vBE, and there will be some nonlinearity.<br />

If R out is large so that iout is always much less than IB , the linearity will<br />

be good, as the operating point will not change significantly over a cycle of the<br />

signal. It is important to keep the peak output current less than the bias current.<br />

This means that<br />

|v o,peak|<br />

R out < IB (6.95)

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