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characterization, modeling, and design of esd protection circuits

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32 Chapter 2. ESD Circuit Characterization <strong>and</strong> Design Issues<br />

log(power)<br />

P α 1/t<br />

P α 1/√t<br />

tc tb ta log(time)<br />

P α 1/log et<br />

P= constant<br />

Fig. 2.12 A qualitative schematic <strong>of</strong> input power-to-failure vs. time-t<strong>of</strong>ailure<br />

predicted by an analytical thermal model.<br />

metal contacts, which are good thermal conductors, <strong>and</strong> the distance between conducting<br />

devices (as in a multiple-finger structure). Nevertheless, the model has been shown to<br />

agree with experimental results to first order.<br />

By carefully stepping the input voltage <strong>and</strong> using varying lengths <strong>of</strong> line, transmissionline<br />

pulsing can be used to capture failure points (as in Fig. 2.10) <strong>and</strong> thus to define a<br />

Pf vs. tf curve <strong>of</strong> an ESD <strong>protection</strong> circuit. The failure power level is the product <strong>of</strong> the<br />

device voltage <strong>and</strong> device current at the point failure occurs (Vt2 <strong>and</strong> It2 ). Since each test<br />

is destructive, several identical devices are needed to extract a curve. If the voltage drop<br />

seen on the oscilloscope is second breakdown (thermal failure), there should be a<br />

significant increase in the measured leakage current after the stress. As discussed in the<br />

previous section, for very short pulse times a significant drop in voltage may not be<br />

observed, in which case it is necessary to define failure as an increase in leakage current

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