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Radio Frequency Integrated Circuit Design - Webs

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

Yc = ic<br />

vc =√2qIC g 2 m<br />

2qIC<br />

g 2 m<br />

Y 2<br />

�<br />

= Y� = j�C�<br />

where it is assumed that r� is not significant. Explicitly,<br />

(6.51)<br />

Gc ≈ 0 (6.52)<br />

Bc = �C�<br />

(6.53)<br />

Thus, the correlation admittance is just equal to the input impedance of the<br />

transistor.<br />

R c , R u , and Gu can also be written down directly.<br />

R c = v 2 c<br />

4kT = 2qIC 4kTg 2 =<br />

m<br />

v T<br />

2IC R u = v 2 u<br />

4kT = 4kTr b<br />

4kT = r b<br />

Gu = i 2 u 2qIB<br />

=<br />

4kT 4kT<br />

= IC<br />

2vT �<br />

(6.54)<br />

(6.55)<br />

(6.56)<br />

Using these equations, an explicit expression for the noise figure can be written<br />

in terms of circuit parameters:<br />

NF = 1 +<br />

IC<br />

2v T � + �G 2<br />

S + (�C� ) 2� v T<br />

2IC<br />

GS<br />

+ G 2<br />

S r b<br />

Here it is assumed that the source resistance has no reactive component.<br />

These equations also lead to expressions for G opt and B opt:<br />

G opt =√<br />

IC<br />

2v T � + r b�− v �2<br />

T<br />

(�C� )<br />

2IC v T<br />

+ r<br />

2I b<br />

C<br />

v T<br />

v T<br />

+ v T<br />

2IC� �C�<br />

2IC<br />

−<br />

v T<br />

2IC (6.57)<br />

�2<br />

(�C� )<br />

+ r b<br />

+ r b<br />

2IC<br />

(6.58)

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