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Radio Frequency Integrated Circuit Design - Webs

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

vo_ncs ≈ R S + Z�<br />

1 + g m Z� incs ≈ re incs<br />

(6.71)<br />

Therefore, the collector shot noise current sees re , a low value, and output<br />

voltage is low. Thus, the common-collector adds little noise to the signal except<br />

through r b .<br />

6.4 Linearity in Amplifiers<br />

Nonlinearity analysis will follow the same basic principles as those discussed in<br />

Chapter 2, with power series expansions and nonlinear terms present in the<br />

amplifier. These will now be discussed in detail.<br />

6.4.1 Exponential Nonlinearity in the Bipolar Transistor<br />

In bipolar transistors, one of the most important nonlinearities present is the<br />

basic exponential characteristic of the transistor itself, illustrated in Figure 6.25.<br />

Source resistance improves linearity. As an extreme example, if the input<br />

is a current source, R S =∞, then i c = �i b . This is as linear as � is. It can be<br />

shown that a resistor in the emitter of value R E has the same effect as a source<br />

or base resistor of value R E �. The transistor base has a bias applied to it and<br />

an ac signal superimposed. Summing the voltages from ground to the base and<br />

assuming that ie = i c ,<br />

vs + VS = v be + VBE + R E (IC + ic ) (6.72)<br />

where VBE and v be are the dc and ac voltages across the base emitter junction<br />

of the transistor.<br />

Figure 6.25 Bipolar common-emitter amplifier for linearity analysis.

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