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Radio Frequency Integrated Circuit Design - Webs

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

Figure 10.43 Transistor with multiple stripes.<br />

to increase current capability, it is possible to use multiple metal layers, for<br />

example, metals 1, 2, and 3. The top metal is often thicker, resulting in a higher<br />

total current capability. In this example, the original 1 mA of current per emitter<br />

stripe might be increased to 4 mA/stripe for 1-�m-wide line. Another point<br />

to keep in mind is that since current flows from collector to emitter, the current<br />

density in the emitters is highest close to the external emitter contact, which<br />

for Figure 10.43 is on the bottom.<br />

10.16 Current Limits in <strong>Integrated</strong> Inductors<br />

<strong>Integrated</strong> inductors as used for LNAs and oscillators are typically 10 or 20<br />

�m wide. This means they can probably handle no more than 20 to 40 mA<br />

of dc current, and maybe up to 80 mA or so of ac current. This obviously<br />

limits the ability to do on-chip tuning or matching for power amplifiers.<br />

10.17 Power Combining<br />

For high power, it is possible to combine multiple transistors at the output as<br />

shown in Figure 10.44. This distributes the heat and limits the current density<br />

in each transistor (compared to a single super-huge transistor).<br />

However, with many transistors, the base drive to the outside transistors<br />

can be phase delayed compared to the shortest path, so it is important to keep<br />

the line lengths equal, as illustrated in Figure 10.44. Note also that as with all<br />

RF or microwave circuits, sharp bends are to be avoided. Line delay or phase<br />

shift can be determined by considering that the wavelength of a 1-GHz sine

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