The Eighth International Conference on Advanced Semiconductor Devices and Microsystems 2010
DOI: 10.1109/asdam.2010.5666319
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Investigation of deep energy levels in heterostructures based on GaN by DLTS

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Cited by 20 publications
(13 citation statements)
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“…The first effect is ascribed to the increase in SRH non-radiative recombination, which reduces the amount of photogenerated hole-electron pairs that can be extracted from the MQW structure. The second effect can be attributed to an increased emission of carriers from the deep levels responsible for yellow luminescence in GaN (EC-0.9 eV), typically carbon [21], VGa-O complexes [22] or VGa-H [23]. By increasing temperature, we also noticed a shift of the band-to-band absorption of the InGaN (edge around 465 nm), that is ascribed to bandgap narrowing.…”
Section: Resultsmentioning
confidence: 75%
“…The first effect is ascribed to the increase in SRH non-radiative recombination, which reduces the amount of photogenerated hole-electron pairs that can be extracted from the MQW structure. The second effect can be attributed to an increased emission of carriers from the deep levels responsible for yellow luminescence in GaN (EC-0.9 eV), typically carbon [21], VGa-O complexes [22] or VGa-H [23]. By increasing temperature, we also noticed a shift of the band-to-band absorption of the InGaN (edge around 465 nm), that is ascribed to bandgap narrowing.…”
Section: Resultsmentioning
confidence: 75%
“…In this device, both Tp1 and Tp2 have been found to be thermally activated with E a = 0.65eVand0.37eV, respectively. Traps with the similar levels have been reported and identified in the GaN buffer close to the interface (~0.6 eV) [29], in heterostructure's interface (0.642 eV) [30], in the GaN film (0.59-0.63 eV) attributed to the edge dislocations by DLTS [31], in AlGaN barrier layer (0.3 eV-0.54e V) detected from transconductance dispersion and admittance curves [26], and in the AlGaN layer (0.37 eV) based on dynamic on-resistance (NDR) [32], respectively. It was suggested that Tp1 in the GaN layer are close to the AlGaN/GaN interface [29][30][31].…”
Section: Detrapping Processesmentioning
confidence: 80%
“…Two time constants representing peaks on the current transient (DP1 and DP2) at 0.45 eV (12 s to 975 s) and 0.65 eV (2 ms to 48 ms) and a valley (TP1) at 0.86 eV (150 ms to 3 s) were measured. These activation energies are associated to C/O/H impurities for DP1 [14], VGa oxygen complex for DP2 [19] and gallium vacancies for TP1 [20] in the literature. The time and thermal windows for DP1 is notably in good concordance with the literature [14].…”
Section: Measurement Results and Discussionmentioning
confidence: 98%