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characterization, modeling, and design of esd protection circuits

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1.1. ESD in the Integrated Circuit Industry 3<br />

1.1 ESD in the Integrated Circuit Industry<br />

Electrical overstress is defined as damage to a product caused by exceeding data-sheet<br />

maximum ratings [10]. EOS usually leads to gross damage in an integrated circuit<br />

resulting from high-energy events such as electrostatic discharge, electromagnetic pulses,<br />

lightning, or reversal <strong>of</strong> power <strong>and</strong> ground pins. EOS failure mechanisms fall into the two<br />

broad categories <strong>of</strong> thermally induced failures <strong>and</strong> high electric-field failures [11]. The<br />

duration <strong>of</strong> an EOS event may be anywhere from less than one nanosecond to one<br />

millisecond <strong>and</strong> longer. Long EOS events can lead to damaged areas such as blown metal<br />

lines, cavities in the silicon, or discoloration <strong>of</strong> silicon due to local heating with a<br />

characteristic radius <strong>of</strong> 100µm or greater [10]. This damage leads to either a reduction in<br />

IC performance (e.g., increased leakage current on one or more pins) or total circuit<br />

failure.<br />

The region <strong>of</strong> EOS phenomena with stress times <strong>of</strong> less than one nanosecond up to a few<br />

hundred nanoseconds is known as electrostatic discharge. (Although EOS covers a large<br />

range <strong>of</strong> phenomena including ESD, it is common to refer to the time range <strong>of</strong> 100ns <strong>and</strong><br />

less as the ESD regime <strong>and</strong> the time range greater than 1µs as the EOS regime, with a sort<br />

<strong>of</strong> transition region from ESD to EOS between 100ns <strong>and</strong> 1µs.) ESD is a relatively rapid,<br />

high-current event resulting from the high voltage created when electrostatic charges are<br />

rapidly transferred between bodies at different potentials. ESD usually leads to relatively<br />

subtle, localized damage sites extending less than 10µm.<br />

As stated previously, there are two main dangers <strong>of</strong> ESD stress. One is the danger <strong>of</strong> gate<br />

oxide dielectric breakdown due to the high voltage seen during an ESD event. In today’s<br />

MOS technologies, gate oxides are on the order <strong>of</strong> 100Å thick, which given an SiO2 dielectric strength <strong>of</strong> 8X10 6 V/cm implies that a stress <strong>of</strong> 8V is enough to cause oxide<br />

damage. In a typical CMOS technology, the thin gates <strong>of</strong> an input buffer are tied directly<br />

to the input pin <strong>and</strong> thus are especially vulnerable to oxide breakdown. Dielectric<br />

breakdown is also <strong>of</strong> concern within the <strong>protection</strong> <strong>circuits</strong> since thin-gate MOS devices<br />

are commonly used. The other form <strong>of</strong> damage created by ESD stress is melting <strong>of</strong><br />

material due to Joule heating, which refers to the resistive heat generated by a current<br />

moving through an electric field ( H =<br />

J ⋅ E,<br />

where H is the heat flow or power density).<br />

If the high current <strong>of</strong> an ESD event is sufficiently localized in an area <strong>of</strong> high electric field,<br />

thermal runaway (also called second breakdown) will result [12,13], leading to either

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