2014
DOI: 10.1063/1.4883317
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Effect of Z1/2, EH5, and Ci1 deep defects on the performance of n-type 4H-SiC epitaxial layers Schottky detectors: Alpha spectroscopy and deep level transient spectroscopy studies

Abstract: Spectroscopic performance of Schottky barrier alpha particle detectors fabricated on 50 lm thick n-type 4H-SiC epitaxial layers containing Z 1/2 , EH 5 , and Ci1 deep levels were investigated. The device performance was evaluated on the basis of junction current/capacitance characterization and alpha pulse-height spectroscopy. Capacitance mode deep level transient spectroscopy revealed the presence of the above-mentioned deep levels along with two shallow level defects related to titanium impurities (Ti(h) and… Show more

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Cited by 41 publications
(16 citation statements)
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“…4. The DLTS measurements are consistent with our previous work 9, 16 on 50 μm n-type 4H-SiC epilayers with the exceptions of peaks 4 and 7 which involve new findings. In total, seven distinct peaks were observed in this study which corresponds to particular defect levels.…”
Section: Resultssupporting
confidence: 93%
“…4. The DLTS measurements are consistent with our previous work 9, 16 on 50 μm n-type 4H-SiC epilayers with the exceptions of peaks 4 and 7 which involve new findings. In total, seven distinct peaks were observed in this study which corresponds to particular defect levels.…”
Section: Resultssupporting
confidence: 93%
“…Deep level capacitance transient spectroscopy is a very sensitive technique to study deep level defects in semiconducting Schottky or p-n junction devices. Figure 20 shows a DLTS spectra obtained for a 50 µm thick n-type Ni/4H-SiC (n-S50) epitaxial Schottky barrier detector in the temperature range 85-790 K [63]. Six well-resolved peaks were observed.…”
Section: Thermally Stimulated Current (Tsc) Measurementsmentioning
confidence: 99%
“…In a capacitance mode DLTS, the system relaxes into equilibrium by thermally emitting the trapped charges after the termination of the filling pulse resulting in capacitance transients. The thermally activated emission rate e n can be expressed as (5) where n is the carrier capture cross section, V th is the mean thermal velocity, N C is the effective density of states, g is the degeneracy of the trap level and was considered to be equal to 1 in the present calculations, and ∆E the energy separation between the trap level and the carrier band. The emission rate is related to the capacitance transient by the following relationship exp (6) where C 0 is the junction capacitance at steady-state reverse bias voltage, and ∆C is the difference in capacitance change Fig.…”
Section: B Defect Characterization By Dltsmentioning
confidence: 99%
“…Among different wide band-gap materials, silicon carbide (SiC) is a promising semiconductor due to its high thermal conductivity, breakdown electrical field, saturation electron drift velocity, and radiation resistance [1][2][3][4][5][6]. 4H-SiC polytype has the most appealing features owing to its comparatively higher band-gap, higher bulk electron mobility, and smaller anisotropy which is suitable for the fabrication of harsh environment compatible nuclear radiation detectors where conventional semiconductors (e.g., Si, Ge, CdTe, CdZnTe) show inadequate performance, though several power devices made of 4H-SiC have outperformed conventional detectors [7]- [13].…”
Section: Introductionmentioning
confidence: 99%
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