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characterization, modeling, and design of esd protection circuits

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108 Chapter 4. Simulation: Calibration <strong>and</strong> Results<br />

A few changes in the simulation structures were made before the final phase <strong>of</strong> calibration<br />

began to more accurately model the non-salicided test structures used for snapback <strong>and</strong><br />

thermal <strong>characterization</strong>. Since the lumped source/drain resistance introduced during the<br />

calibration <strong>of</strong> the drain characteristics was unreasonably large, it was removed from the<br />

simulation model. This simplifies the simulation-structure specification <strong>and</strong> is justified<br />

because the new, salicide-blocked test structures are at least 2.5 times wider than the<br />

previous structures, which implies much more contact area <strong>and</strong> thus less contact<br />

resistance, <strong>and</strong> because the package leads are ultrasonically bonded to the contact pads,<br />

introducing minimal series resistance. Since the new structures make use <strong>of</strong> a salicide<br />

mask, the simulated source <strong>and</strong> drain contacts are placed at the same distance from the<br />

gate as in the actual structures, in contrast to the minimal contact spacing used for the fully<br />

salicided structures in the previous subsection. This contact-to-gate spacing varies from<br />

3µm to 8µm on the drain <strong>and</strong> source sides in the test structures <strong>and</strong> simulations. The<br />

I device / mA<br />

600<br />

400<br />

200<br />

+<br />

V in<br />

-<br />

50Ω<br />

50Ω<br />

Idevice Vdevice 0<br />

0 3 6 Vsb 9 12 15<br />

V device / volts<br />

1/R sb<br />

Fig. 4.41 I-V points from the transmission-line pulse sweep <strong>of</strong> a st<strong>and</strong>ard<br />

50 ⁄ 0.75µm test structure (equivalent circuit shown inset). The trigger<br />

voltage (Vt1 ), snapback voltage (Vsb ), snapback resistance (Rsb ), <strong>and</strong><br />

second-breakdown point (Vt2 , It2 ) can be extracted from the curve.<br />

V t1<br />

V t2 , I t2

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