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CMOS Optical Preamplifier Design Using Graphical Circuit Analysis

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Pole frequencies(MHz)<br />

500<br />

450<br />

400<br />

350<br />

300<br />

250<br />

200<br />

150<br />

100<br />

50<br />

5.2 Developing an Analytic <strong>Circuit</strong> Model 129<br />

Since the process of optimizing the frequency response involves maximizing the<br />

gain for a desired bandwidth, the gain-bandwidth (GBW) product is a useful figure<br />

of merit because it combines gain and bandwidth into a single quantity. Although<br />

bandwidth and gain can be traded off with feedback, the product of the two is often<br />

fixed for a given topology, bias condition, etc. We can optimize our preamplifier<br />

design through maximizing the GBW. By approximating the bandwidth with ω p1 ,<br />

we can obtain an analytic expression for the GBW from Equations (5.25) and<br />

(5.26):<br />

0<br />

0 5<br />

R (kΩ)<br />

f<br />

10 15<br />

500<br />

450<br />

400<br />

350<br />

300<br />

250<br />

200<br />

150<br />

100<br />

0<br />

20<br />

Figure 5.20 shows the resulting 3-dimensional plot of GBW versus and<br />

(5.30)<br />

while Figure 5.21 presents the same surface in two, 2-dimensional projections<br />

views. Across the design space, we see that the GBW can vary by over an order of<br />

magnitude. We can identify that portion of the design space which meets our band-<br />

width requirement by projecting the bounded region identified in Figure 5.18 onto<br />

the GBW plot. Within this region, we have marked in grey a sub-region that corre-<br />

sponds to an area with the highest GBW.<br />

Pole frequencies(MHz)<br />

50<br />

10<br />

0 −10<br />

20*log (K )<br />

10 cm<br />

Figure 5.19 Two projections of the surface plot in Figure 5.18.<br />

GBW<br />

( gm1 + gs1) ( 1 – gm3 R f )<br />

= ----------------------------------------------------------------------------------------------<br />

Cin + ( gm1 + gs1) ( CL + C f )Rf⁄ K cm<br />

−20<br />

surface —<br />

mesh —<br />

R f<br />

ω p1<br />

ωo K cm

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