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III. Gm-C Filtering - Epublications - Université de Limoges

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APPENDIX D<br />

D.1 MOS Differential Pair<br />

The following study is based on computations that may be found in [D.1] and [D.2].<br />

D.1.a Transfer Characteristic<br />

Let’s consi<strong>de</strong>r the MOS differential pair <strong>de</strong>picted in Figure 205. It is also assumed that<br />

M1 and M2 are in the strong inversion regime and in saturation mo<strong>de</strong>.<br />

Hence,<br />

Assuming that<br />

Figure 205. Simplified Transconductor<br />

W<br />

β = μCox<br />

(D.1)<br />

L<br />

and the same β for M1 and M2, currents I1 and I2 are given by:<br />

1<br />

I1 = β<br />

2<br />

1 c −<br />

1<br />

2<br />

2 c<br />

2<br />

V E E I − − = β<br />

( ) 2<br />

V E E −<br />

- 212 -<br />

th<br />

( ) 2<br />

1<br />

I 1 = β 1 c −<br />

2<br />

th<br />

( E − E V )<br />

I 2 =<br />

1<br />

β ( E 2 − Ec<br />

2<br />

−Vth<br />

)<br />

It is also consi<strong>de</strong>red the differential current Imd, <strong>de</strong>fined as follows:<br />

th<br />

(D.2)<br />

(D.3)<br />

(D.4)<br />

(D.5)

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