AVS 64th International Symposium & Exhibition | |
Scanning Probe Microscopy Focus Topic | Tuesday Sessions |
Session SP+AS+MI+NS+SS-TuA |
Session: | Probe-Sample Interactions |
Presenter: | Yasuo Cho, Tohoku University, Japan |
Authors: | N. Chinone, Tohoku University, Japan Y. Cho, Tohoku University, Japan |
Correspondent: | Click to Email |
Physical properties of metal-oxide-semiconductor (MOS) interface are critical for semiconductor devices. There are several techniques for characterizing MOS interface properties. Deep level transient spectroscopy (DLTS)is one of powerful techniques capable of macroscopic quantitative evaluation of trap density at/near MOS interface (Dit). But it is easily imagined that actual trap is not homogeneously distributed, but has two dimensional distributions in atomic scale and even in mesoscopic scale. Therefore, it is very important to characterize MOS interface microscopically. Unfortunately, it is impossible to observe such inhomogeneity by using conventional macroscopic DLTS method.
In this paper, a new technique for local DLTS imaging based on scanning nonlinear dielectric microscopy (SNDM) is proposed. This method enables us to observe two dimensional distribution of trap density at/near MOS interface and is demonstrated with oxidized SiC wafer.
45-nm-thick thermal oxide layers were formed on three Si-faces of 4°-off n-type 4H-SiC wafers. One of them was labeled as #S-45-1. The other two wafers were subjected to post-oxidation annealing (POA) in nitric oxide (NO) at different conditions as follows: 1250°C for 10 minutes (#S-45-2), 1150°C for 60 minutes (#S-45-3). The average Dit values of these samples were measured by conventional High-Low method, which showed that the Dit of #S-45-1 was highest and that of #S-45-3 was lowest.
These three samples were scanned on 1.5x1.5μm2 square area with a resolution of 30x30 pixels and analyzed using the proposed local DLTS method.
By analyzing the acquired images, time-constant τ and magnitude of transient capacitance response were obtained at each pixel. Highest brightness was obtained from #S-45-1 and lowest one was obtained from #S-45-3, which is consistent with macroscopically obtained result. Furthermore, in the local DLTS images, we detected dark and bright areas, which can be translated as two dimensional trap distribution.
Next, quantitative imaging of Dit was performed. Distributions of Dit for τ = 0.3 μs and 3 μs were imaged for all samples. The time constants 0.3 μs and 3 μs correspond to energy depth of 0.24 eV and 0.30 eV below the conduction band, respectively. All images have dark and bright areas with feature size of a few 100 nm. In addition, the images with different time constant showed different distribution, which implies that the distribution of interface traps depends on time constant, or suggests the physical origin of interface trap with different energy level is different.
This local DLTS technique can contribute to understanding microscopic physical properties of MOS interface.