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characterization, modeling, and design of esd protection circuits

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6.1. Contributions 167<br />

TLP was shown to be a powerful tool for extracting the critical I-V parameters <strong>of</strong> ESD test<br />

structures fabricated in a leading-edge CMOS technology. A discussion was given on the<br />

dependence <strong>of</strong> these critical I-V parameters on process <strong>and</strong> layout parameters. Testing<br />

focused on structures with varying widths <strong>and</strong> contact-to-gate spacings, <strong>and</strong> power to<br />

failure <strong>and</strong> current to failure were measured between 50ns <strong>and</strong> 600ns. The usefulness <strong>of</strong><br />

the extracted I-V parameters <strong>and</strong> failure levels was demonstrated in the application <strong>of</strong> the<br />

ESD <strong>design</strong> methodology to SRAM <strong>circuits</strong>.<br />

6.1.2 Numerical Device Simulation<br />

Lattice-temperature <strong>modeling</strong> in 2D numerical device simulation <strong>and</strong> the temperaturedependent<br />

models required for proper <strong>modeling</strong> <strong>of</strong> high-temperature effects associated<br />

with ESD were reviewed. New simulation methods were presented, including a generalpurpose<br />

curve-tracing algorithm, developed <strong>and</strong> implemented as a C program, which<br />

guides a simulator through complex I-V curves. The curve tracer’s application to ESD was<br />

demonstrated in the control <strong>of</strong> dc snapback simulations. More general applications <strong>of</strong> the<br />

curve tracer <strong>and</strong> a user’s manual are presented as an appendix. A quantitative analysis was<br />

conducted to compare <strong>and</strong> contrast the 2D <strong>and</strong> 3D formulations <strong>of</strong> an analytic thermal<br />

model which, to first order, describes the heating <strong>of</strong> a device during an ESD event. The<br />

results <strong>of</strong> the analysis predict that for stress times in the ESD <strong>and</strong> EOS regimes, the power<br />

to failure modeled in two dimensions will be higher than that <strong>of</strong> the three-dimensional<br />

model or <strong>of</strong> an actual device. This directly conflicts the conclusions reached in previous<br />

studies <strong>of</strong> electrothermal simulation that 2D simulations underestimate the power to<br />

failure. Methods for studying dielectric failure <strong>and</strong> latent damage with 2D simulation were<br />

proposed, including monitoring <strong>of</strong> hot-carrier injection <strong>and</strong> hot-spot spreading during an<br />

ESD simulation.<br />

A procedure for calibrating simulation models for use in quantitative ESD simulations<br />

was delineated, including structure definition <strong>and</strong> determination <strong>of</strong> mobility <strong>and</strong> impactionization<br />

model coefficients <strong>and</strong> thermal boundary conditions. I-V <strong>and</strong> failure<br />

characteristics <strong>of</strong> st<strong>and</strong>ard test structures were used as the basis <strong>of</strong> the calibration. While<br />

quantitative <strong>modeling</strong> <strong>of</strong> the snapback I-V parameters was achieved, <strong>modeling</strong> <strong>of</strong> thermal<br />

failure was inadequate due to unresolved issues regarding <strong>modeling</strong> <strong>of</strong> the electric field at<br />

high current levels in the drain junction region, where the device physics are most critical<br />

<strong>and</strong> most complex. Usefulness <strong>of</strong> the ESD snapback simulations was nonetheless

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