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characterization, modeling, and design of esd protection circuits

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5.2. Application 155<br />

To determine how to best describe the layout dependence <strong>of</strong> the withst<strong>and</strong> current <strong>and</strong><br />

voltage using a second-order linear model, single-factor trends are examined for DGS,<br />

SGS, n, <strong>and</strong> W. In Fig. 5.56, the normalized VHBM,ws vs. DGS line has a negative<br />

curvature, indicating that the ITLP,ws <strong>and</strong> VHBM,ws model equations should have quadratic<br />

as well as linear DGS terms, with the quadratic terms being negative. A quadratic<br />

dependence on SGS is also observed, but over the limited range <strong>of</strong> the <strong>design</strong> space (2.2 to<br />

4.2µm) a linear term is adequate. As seen in Fig. 5.57, the normalized failure parameters<br />

have an inverse dependence on the number <strong>of</strong> fingers, <strong>and</strong> consequently these parameters<br />

are not well described using linear <strong>and</strong> quadratic n (number-<strong>of</strong>-finger) factors. However, if<br />

1/n is chosen as the factor, a good fit is obtained with just a linear term. Since the<br />

normalized ITLP,ws <strong>and</strong> VHBM,ws also have an inverse dependence on width, 1/W is<br />

chosen as a factor, but in this case the best fit is obtained by also including a quadratic<br />

term. Finally, we assume that SGS does not interact with any <strong>of</strong> the factors since its value<br />

does not vary widely, but the three interaction terms between DGS, 1/n, <strong>and</strong> 1/W are<br />

included. The resulting withst<strong>and</strong>-current model is<br />

ITLP, ws<br />

----------------- = c<br />

( Wn)<br />

0 c1( SGS)<br />

c2 ( DGS)<br />

c3 ( DGS)<br />

2<br />

+ + + + c4 ( 1⁄ n)<br />

+ c5 ( 1 ⁄ W)<br />

c6 ( 1 ⁄ W)<br />

2<br />

+ + c7 ( DGS)<br />

( 1 ⁄ n)<br />

+ c8 ( DGS)<br />

( 1 ⁄ W)<br />

+ c9 ( 1 ⁄ n)<br />

( 1 ⁄ W)<br />

(5.53)<br />

with an identical equation (with different coefficient values) for VHBM,ws . Note that the<br />

constant coefficient, c0 , lumps together the constant terms from the separate factor<br />

dependencies.<br />

Model coefficients for Eqs. (5.51)-(5.53) were extracted using Catalyst for two<br />

development lots with slightly different process recipes. HBM <strong>and</strong> 150ns TLP<br />

<strong>characterization</strong> <strong>of</strong> the <strong>design</strong> space was performed on two wafers per lot <strong>and</strong> five die sites<br />

per wafer, with average response values <strong>of</strong> each structure used as the Catalyst input.<br />

SRAM test <strong>circuits</strong> from the same wafers were submitted to the AMD Reliability<br />

Laboratory for HBM stressing <strong>of</strong> I/O vs. VSS , I/O vs. VCC , <strong>and</strong> VCC vs. VSS pin<br />

combinations to determine average, i.e., not qualification, HBM withst<strong>and</strong> voltages.<br />

Results for the two lots are summarized in Table 5.2. For each lot, the layout parameters <strong>of</strong><br />

each stressed circuit were plugged into the ITLP,ws model equation to determine the<br />

mA ⁄<br />

µm values in Table 5.2. These values were then converted to VHBM,ws values by

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