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Radio Frequency Integrated Circuit Design - Webs

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

where<br />

The pole and zero are given by<br />

if g m R E >> 1, then<br />

and<br />

f z1 ≈ g m<br />

C� =−� T<br />

f p1 ≈−<br />

1<br />

C� R A<br />

R A = r� || R B + R E<br />

1 + g m R E<br />

R A ≈ R B + R E<br />

g m R E<br />

R E<br />

f p1 ≈−<br />

R E + R B<br />

� T<br />

(6.19)<br />

(6.20)<br />

(6.21)<br />

(6.22)<br />

(6.23)<br />

The input impedance of this amplifier can also be determined. If g m R E<br />

>> 1, then we can use the small-signal circuit to find Z in. The input impedance,<br />

again ignoring C� , is given by<br />

Z in = Z� + R E (1 + g m Z� ) (6.24)<br />

Likewise, the output impedance can be found and is given by<br />

Z out = r� + R B + sC� r� R B<br />

1 + g m r� + sC� r�<br />

(6.25)<br />

Provided that r� > R B and �C� r� > r� at the frequency of interest, the<br />

output impedance simplifies to<br />

1 + g m R B j� /�T<br />

Z out ≈ re<br />

1 + j� /�T<br />

(6.26)

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