4.6 One-Dimensional Source/Drain Doping Profiling



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4.6 One-Dimensional Source/Drain Doping Profiling

For an abrupt PN junction with a step doping on the high concentration side,   the deep depletion approximation results in similar equations to   (4.6) and (4.7) for the value of the doping concentration on the low side:

 

and

 

where is the distance from the junction and is the reverse junction depletion capacitance per unit area. CV profiling can only yield the doping on one side of the junction. For this reason, the profile of the high concentration side should be determined using direct measurement techniques such as secondary ion mass spectroscopy (SIMS) or incremental spreading resistance (SRP). Both methods     provide reasonable accuracy for this type of profile measurements. The logarithm of the measured concentration is then fitted by a B-spline   function using least-squares approximation.

An initial guess for the low side doping profile is calculated by performing the analytical extraction using (4.9) and (4.10). The analytical profile is defined from the junction location to the extent of the depletion region corresponding to the maximum reverse junction applied. For convenience, it is extended uniformly by adding a knot at the silicon surface. The coefficient of this knot is not included in the optimization since the doping at this position is compensated by the doping of the high concentration side. The same algorithm as described in Section 4.5.1 can be used to automatically determine the B-spline partition during the inverse modeling extraction.





Martin Stiftinger
Tue Aug 1 19:07:20 MET DST 1995