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characterization, modeling, and design of esd protection circuits

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

voltage, VT [41]. The reduction in Vt1 ranges from a few volts for small gate-length<br />

devices to about 50% for larger gate lengths. Beyond VT , the trigger voltage levels <strong>of</strong>f<br />

with increased gate biasing <strong>and</strong> may actually increase since the reduced electric field in<br />

the drain depletion region will reduce impact ionization. If the gate remains biased after<br />

a device has entered snapback, It2 can be reduced due to concentration <strong>of</strong> drain-source<br />

current at the surface <strong>of</strong> the channel, so it is important that the gate be biased only<br />

during initial turn-on <strong>of</strong> the device.<br />

• LDD -- It is generally assumed that a lightly doped drain decreases the performance <strong>of</strong><br />

an ESD <strong>protection</strong> structure because it has a much lower junction depth than the S/D<br />

diffusion, which leads to higher current concentrations in the area <strong>of</strong> high electric field<br />

(i.e., the box depth is smaller in the 3D thermal model) <strong>and</strong> thus reduces It2 . However,<br />

if the LDD depth is not much different than the S/D depth, then there should be little<br />

change in It2 unless the accompanying change in the electric-field pr<strong>of</strong>ile is significant.<br />

In a CMOS process the NMOS LDD implant can be blocked simply by covering the<br />

NMOS active area with the same oxide used to mask the PMOS active areas during this<br />

implant. Of course, the spacer oxide will still be present after the oxide etch, which<br />

means the S/D diffusion edges will be separated from the intrinsic channel under the<br />

gate contact, i.e., the gate length is effectively increased by twice the spacer width.<br />

(Since it is only the drain side <strong>of</strong> the device which has the high electric field, the source<br />

LDD diffusion may be left in the process, meaning the gate length is only increased by<br />

one spacer width.) Thus, blocking the LDD implant also effects the same changes as<br />

increasing the gate length. These effects may be compensated by reducing the drawn<br />

gate length. Although the drain junction may become more abrupt when the LDD is<br />

omitted, Vbd increases because the net drain doping decreases without the LDD<br />

implant, <strong>and</strong> therefore Vt1 <strong>and</strong> Vsb also increase. The snapback resistance will also<br />

probably be slightly larger due to the increased effective gate length.<br />

• Substrate resistance -- Increasing the substrate resistance, either by moving the substrate<br />

contact farther away from the drain diffusion or by adding a lumped resistance<br />

between the local substrate contact <strong>and</strong> ground, or floating the substrate accelerates the<br />

onset <strong>of</strong> snapback by creating a higher substrate bias for the same substrate current <strong>and</strong><br />

by diverting more <strong>of</strong> the impact-ionization generated holes toward the source to forward<br />

bias the source-substrate junction. The reduction in Vt1 <strong>and</strong> It1 imply a faster triggering<br />

<strong>of</strong> the device. To first order, the snapback region <strong>of</strong> operation is not affected by

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