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characterization, modeling, and design of esd protection circuits

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

log(I leak / A)<br />

-3<br />

-6<br />

-9<br />

-12<br />

0 It1 1<br />

Idev / A<br />

It2 2<br />

Fig. 2.13 Qualitative plot <strong>of</strong> device leakage evolution vs. stress-current<br />

level <strong>of</strong> a TLP experiment. Transitions are evident at the<br />

snapback <strong>and</strong> second-breakdown points.<br />

drain-substrate junction, <strong>and</strong>/or a rupture <strong>of</strong> the gate oxide. In addition to this transition,<br />

sudden increases in leakage from the pA to the nA range have been observed when the<br />

device enters snapback [4]. Such a leakage evolution is depicted in Fig. 2.13 by plotting<br />

leakage current vs. the device current <strong>of</strong> the previous TLP stress. Non-catastrophic<br />

leakage (also called low-level leakage or s<strong>of</strong>t failure) may be due to a small hot spot<br />

forming just before the device snaps back, to a small filament in the gate oxide formed by<br />

dielectric stress, or to hot-carrier trapping in the gate oxide which could induce a small<br />

channel region by shifting the threshold voltage below zero (for an NMOS device).<br />

Although the <strong>protection</strong> circuit still functions after a low-level stress, the increased<br />

leakage may be a signature <strong>of</strong> a latent failure, i.e., a reduction in lifetime <strong>of</strong> the circuit due<br />

to a “s<strong>of</strong>t” ESD stress. Latent failure is a topic which merits further investigation, <strong>and</strong> the<br />

monitoring <strong>of</strong> leakage current during stepped TLP stresses is a powerful way to study the<br />

phenomenon.

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