Abstract:Deep levels by proton and electron irradiation in 4H-SiC J. Appl. Phys. 98, 053706 (2005); 10.1063/1.2014941 Electrically active defects in irradiated 4H-SiC J. Appl. Phys. 95, 4728 (2004); 10.1063/1.1689731Evidence for negatively charged vacancy defects in 6H-SiC after low-energy proton implantation Low temperature annealing of 4H-SiC Schottky diode edge terminations formed by 30 keV Ar + implantation
“…The bistable M-center with its two configurations A and B is detected. As discussed by Martin et al 8,9 and as can be seen from Fig. 1, the M-center is superimposing the EH1, Z 1=2 , and EH3 peaks.…”
Section: Resultsmentioning
confidence: 81%
“…The amplitudes are similar for M1 and M2 and slightly less for M3 because M2 and M3 are overlapping and thus partly cancel out during subtraction. Martin et al 8 and Nielsen et al, 10 attributed M1 and M3 to the same defect configuration but different charge states and M2 to another defect configuration. Because the M-center is detected after low-energy irradiation, it may be attributed to carbon related defects.…”
Section: Resultsmentioning
confidence: 99%
“…The origin of these peaks were attributed to a highly mobile defect, recombining at rather low temperatures. In 2 MeV proton-implanted n-type 4H-SiC, a bistable defect, the M-center, 8 was observed. The defect has two configurations A and B.…”
After low-energy electron irradiation of epitaxial n-type 4H-SiC with a dose of 5 Â 10 16 cm À2 , the bistable M-center, previously reported in high-energy proton implanted 4H-SiC, is detected in the deep level transient spectroscopy (DLTS) spectrum. The annealing behavior of the M-center is confirmed, and an enhanced recombination process is suggested. The annihilation process is coincidental with the evolvement of the bistable EB-centers in the low temperature range of the DLTS spectrum. The annealing energy of the M-center is similar to the generation energy of the EB-centers, thus partial transformation of the M-center to the EB-centers is suggested. The EB-centers completely disappeared after annealing temperatures higher than 700 C without the formation of new defects in the observed DLTS scanning range. The threshold energy for moving Si atom in SiC is higher than the applied irradiation energy, and the annihilation temperatures are relatively low, therefore the M-center, EH1 and EH3, as well as the EB-centers are attributed to defects related to the C atom in SiC, most probably to carbon interstitials and their complexes.
“…The bistable M-center with its two configurations A and B is detected. As discussed by Martin et al 8,9 and as can be seen from Fig. 1, the M-center is superimposing the EH1, Z 1=2 , and EH3 peaks.…”
Section: Resultsmentioning
confidence: 81%
“…The amplitudes are similar for M1 and M2 and slightly less for M3 because M2 and M3 are overlapping and thus partly cancel out during subtraction. Martin et al 8 and Nielsen et al, 10 attributed M1 and M3 to the same defect configuration but different charge states and M2 to another defect configuration. Because the M-center is detected after low-energy irradiation, it may be attributed to carbon related defects.…”
Section: Resultsmentioning
confidence: 99%
“…The origin of these peaks were attributed to a highly mobile defect, recombining at rather low temperatures. In 2 MeV proton-implanted n-type 4H-SiC, a bistable defect, the M-center, 8 was observed. The defect has two configurations A and B.…”
After low-energy electron irradiation of epitaxial n-type 4H-SiC with a dose of 5 Â 10 16 cm À2 , the bistable M-center, previously reported in high-energy proton implanted 4H-SiC, is detected in the deep level transient spectroscopy (DLTS) spectrum. The annealing behavior of the M-center is confirmed, and an enhanced recombination process is suggested. The annihilation process is coincidental with the evolvement of the bistable EB-centers in the low temperature range of the DLTS spectrum. The annealing energy of the M-center is similar to the generation energy of the EB-centers, thus partial transformation of the M-center to the EB-centers is suggested. The EB-centers completely disappeared after annealing temperatures higher than 700 C without the formation of new defects in the observed DLTS scanning range. The threshold energy for moving Si atom in SiC is higher than the applied irradiation energy, and the annihilation temperatures are relatively low, therefore the M-center, EH1 and EH3, as well as the EB-centers are attributed to defects related to the C atom in SiC, most probably to carbon interstitials and their complexes.
“…There have been several investigations on both high-energy irradiated [18][19][20][21][22][23] and low-energy irradiated [24][25][26] SiC. In a recent study [15], we discussed the annealing of EH1, EH3 and the bistable M-center, which was discovered and labelled by Martin et al [12], as well as the related formation of the bistable EB-centers in low-energy irradiated SiC, which were discovered and labelled by Beyer et al [14]. Finally, the annihilation of the EB-centers at about 700 • C and their association with carbon interstitials and/or related complexes were reported.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, several bistable [12][13][14][15] and multistable [16] defects have also been reported in the SiC for its polytypes 4H-and 6H-SiC, respectively. In 6H-SiC, Hemmingsson et al [16] investigated a metastable defect with three different configurations.…”
The energy needed to conduct the transformations were determined to E A (A → B) = (2.1 ± 0.1) eV and E A (B → A) = (2.3 ± 0.1) eV, respectively. The pre-factor indicated an atomic jump process for the opposite transition A → B and a charge carrieremission dominated process in case of B → A. Minority charge carrier injection enhanced the transformation from configuration B to configuration A by lowering the transition barrier by about 1.4 eV. Since the bistable FB-center is already present after low-energy electron irradiation (200 keV), it is likely related to carbon.
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