“…2(b) due to the fast sweep-out of free carriers in the re-established SCR region. At this point, the trapped electrons (nTc) in the SCR compensate part of the ionized donors [7,[24][25][26][27], so that the effective junction capacitance (CR) reduces after the end of the filling pulse [25] (3) where ND + is the ionized donor concentration, A is the diode active area, q is the elementary charge, and Vbi is the built-in voltage of the SBD. If the trapped electrons gain sufficient thermal energy (Ea > EC -ET), they are emitted from the trap level to the conduction band and subsequently swept out by the applied electric field.…”
Section: Fundamentals Of Dltsmentioning
confidence: 99%
“…Thermally stimulated capacitance (TSCAP) [24][25][26][27] spectroscopy measurements are performed to complement the DLTFS results. The carrier capture and emission kinetics are evaluated by conducting isothermal transient spectroscopy (ITS) [13] at a stabilized temperature.…”
“…2(b) due to the fast sweep-out of free carriers in the re-established SCR region. At this point, the trapped electrons (nTc) in the SCR compensate part of the ionized donors [7,[24][25][26][27], so that the effective junction capacitance (CR) reduces after the end of the filling pulse [25] (3) where ND + is the ionized donor concentration, A is the diode active area, q is the elementary charge, and Vbi is the built-in voltage of the SBD. If the trapped electrons gain sufficient thermal energy (Ea > EC -ET), they are emitted from the trap level to the conduction band and subsequently swept out by the applied electric field.…”
Section: Fundamentals Of Dltsmentioning
confidence: 99%
“…Thermally stimulated capacitance (TSCAP) [24][25][26][27] spectroscopy measurements are performed to complement the DLTFS results. The carrier capture and emission kinetics are evaluated by conducting isothermal transient spectroscopy (ITS) [13] at a stabilized temperature.…”
“…Among the traditional methods for electrical analysis of these defect characteristics, Capacitance Deep Level Transient Spectroscopy (CDLTS) [1] is the best known. The principle of the CDLTS capturing or emitting charge carriers at deep levels has also been adopted in many ways to Optical DLTS [2][3][4][5], Photoinduced Current Transient Spectroscopy (PICTS) [6][7][8][9][10], Fourier Transform (FT)-DLTS [11][12][13], Laplace Transform (LT)-DLTS [14][15][16], Charge based (Q)-DLTS [17][18][19][20], etc., according to the measurement environment and sample conditions. However, the analysis methods mentioned above are typically performed over a very wide temperature range (e.g., (60-400) K) using very short temperature intervals (e.g., 1 K) over very long periods of time (e.g., several hours in some cases, and over 12 h in specific cases).…”
We propose and demonstrate that temperature-dependent curve-fitting error values of the Schottky diode I–V curve in the forward regime can be an auxiliary diagnostic signal as the temperature-scan Capacitance DLTS (CDLTS) signals and helps to work time-efficiently with high accuracy when using the Laplace Transform (LT)–DLTS or Isothermal Capacitance transient spectroscopy (ICTS) method. Using Be-doped GaAs showing overlapping DLTS signals, we verify that the LT–DLTS or ICTS analysis within a specific temperature range around the characteristic temperature Tpeak coincides well with the results of the CDLTS and Fourier Transform DLTS performed within the whole temperature range. In particular, we found that the LT–DLTS signals appeared intensively around Tpeak, and we confirmed it with the ICTS result. The occurrence of the curve fitting error signal is attributed to the relatively increased misfit error by the increased thermal emission from the deep-level trap in the case near the Tpeak, because the applied transport model excludes defect characteristics.
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