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characterization, modeling, and design of esd protection circuits

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3.7. Simulation <strong>of</strong> Dielectric Failure <strong>and</strong> Latent ESD Damage 87<br />

E max (10 6 V/cm) <strong>and</strong> V d (V)<br />

24<br />

20<br />

16<br />

12<br />

8<br />

4<br />

0<br />

0<br />

+<br />

V in<br />

-<br />

50Ω<br />

50Ω<br />

V d<br />

E max<br />

1.0 2.0 3.0 4.0<br />

time / ns<br />

Fig. 3.34 The maximum electric field in the gate oxide (E max , in MV/cm) <strong>of</strong> an<br />

ESD-<strong>protection</strong> MOSFET subjected to a square pulse with a 3ns rise time<br />

is plotted vs. time. As seen from the plot <strong>of</strong> the input voltage at the drain<br />

<strong>of</strong> the device, V d , the reduction in E max is due to the device snapping back<br />

at 1.2ns.<br />

injection <strong>of</strong> charge into the oxide <strong>and</strong> high electric-field stress across the oxide (these are<br />

not necessarily mutually exclusive). The simplest analysis <strong>of</strong> dielectric stress during ESD<br />

involves recording the voltage across the gate oxide or the maximum electric field in the<br />

oxide <strong>of</strong> the <strong>protection</strong> transistor for each solution in a transient or steady-state snapback<br />

simulation. The device simulator does not report such voltage <strong>and</strong> electric-field<br />

information directly, but the desired information can be extracted from files containing the<br />

2D potential <strong>and</strong> electric-field pr<strong>of</strong>iles saved from each solution. Fig. 3.34 shows a plot <strong>of</strong><br />

the simulated maximum electric field vs. time in the 100Å-thick oxide <strong>of</strong> a <strong>protection</strong><br />

MOSFET subject to a square-wave pulse with a 3ns rise time. The simulator was<br />

instructed to save the solution data for each time point, <strong>and</strong> the location <strong>and</strong> value <strong>of</strong> the<br />

maximum electric field in the device were then automatically extracted from each solution<br />

using a simple C program. Fig. 3.34 shows that the maximum electric field peaks at a<br />

V d<br />

5.0

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