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edfas.org 25 ELECTRONIC DEV ICE FA I LURE ANALYSIS | VOLUME 24 NO . 1 the V peak values obtained from forward and backward d C /d V - V signals. Thus, V peak is the point of inflection in the CV data and changes in this value reflect the voltage shift in CV characteristics. As noted, the value of Δ V peak indicates the degree of hysteresis in the data. The reconstructed V peak results obtained from the backward and forward data are shown in Figs. 7a and 7b, while Figs. 7c and 7d respectively provide Δ V peak and D it images acquired from a specimen without POA. These real-space images exhibit an inhomogeneous distribu- tion of clusters, which has been previously observed in local DLTS and SNDM images. The evident variations in the V peak values in Figs. 7a and 7b have been attributed to nonuniform in-plane SiO 2 /SiC interface surface poten- tials. [21] These fluctuations in potential are associatedwith spatially inhomogeneous current and carrier densities in SiCMOS devices. Prior simulations by our group based on actual tr-SNDM D it images have predicted such results. [22] It has also been proposed that a nonuniform interface can potentially result in limited channel mobility. [21,22] Finally, the variations in the Δ V peak values in Fig. 7c reflect a nonuniform distribution of D it . CONCLUSION This article introduced and explained tr-SNDM, a newly developed digital version of SNDM, after briefly discuss- ing the application of conventional analog type SNDM to the assessment of semiconductors. The performance of tr-SNDM was demonstrated by simultaneously acquiring nanoscale local CV, d C /d V - V , and local DLTS data from insulator-semiconductor interfaces. This technique is applicable to the analysis of SiO 2 /SiC interfaces such as those found in power electronics, and the present exami- nation of spatial fluctuations in different images indicates the possibility that intrinsic nonuniformity persists at SiO 2 /SiC interfaces. 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