165 160 155 --~ 150 ,~ 145 ~= 140 ~ 135 125 120 115 110 Y. Electrochem. S oc.: SOLID-STATE SCIENCE AND TECHNOLOGY A 1.0 1.2 1.4 1.6 1.8 2.0 2.2 2.4 2.6 2.8 3.0 PROBE RADIOS {p,m] Fig. 12. A series of plots of the results of the calibration investigation for several values of the probe spacing. The values of the probe spacings and the corresponding curves are: S ~-25 ~m (A), S = 50 ~rn (B), S = 75 #m (C), and S = 100 ~m (D). In all cases, the Berkowitz-Lux correction factor scheme was used.sufficient to provide sensitivity and yield the value of a = 2 ~an, which was originally used in the generation of the spreading resistance. In addition, to show that the sensitivity is not degraded by variation of the probe spacing, the results of the analysis for several values of the probe spacing are presented in Fig. 12. It is important to emphasize that the curvature must be sufficient to provide for the evaluation of the value of a. Should the curve be found to be flat, this would preclude the use of this procedure.
Conclusions