2018
DOI: 10.1109/ted.2018.2849501
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Characterization of Buffer-Related Current Collapse by Buffer Potential Simulation in AlGaN/GaN HEMTs

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Cited by 37 publications
(28 citation statements)
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“…The polarization scale parameter with 0.29 has been applied to be consistent with the measured experimental data [12]. Shockley-Read-Hall and Fermi-Dirac statistics are enabled to simulate the trapping and de-trapping mechanisms under different voltage stresses [25,26]. The self-heating effect including the lattice temperature model and electron/hole thermal model is enabled to monitor possible hole/electron emission processes [27].…”
Section: Sentaurus Device Simulation Resultsmentioning
confidence: 99%
“…The polarization scale parameter with 0.29 has been applied to be consistent with the measured experimental data [12]. Shockley-Read-Hall and Fermi-Dirac statistics are enabled to simulate the trapping and de-trapping mechanisms under different voltage stresses [25,26]. The self-heating effect including the lattice temperature model and electron/hole thermal model is enabled to monitor possible hole/electron emission processes [27].…”
Section: Sentaurus Device Simulation Resultsmentioning
confidence: 99%
“…The focus is mainly on the E-mode mechanism as well as the methods of increasing the threshold voltage of the HEMTs [134,135]. And the simulations have also been used to study the gate leakage current [136,137], the device reliability [138], the short channel effects [139], current collapse [140] and so forth. For the simulation of the AlGaN/GaN HEMTs, the most important work is to solve the 2DEG concentration which is generated by spontaneous polarization (P sp ) and piezoelectric polarization (P pe ) [141], as shown in Figure 8.…”
Section: Algan/gan Device Simulationmentioning
confidence: 99%
“…The reason may be that some of those papers neglect the initial state of GaN HEMTs with bias stress. Previous work has shown that a GaN device always operates at a certain quiescent bias when the heterostructure under the gate-metal along with the buffers of the GaN devices capture charges, which will serve as an important condition to cause the threshold voltage roll-off [24], [27], [34]. Another reason may be that those dispersive phenomena cannot follow the applied signal at high frequencies because of much longer de-trapping time constants (usually more than hundreds of microsecond) than the reciprocal of microwave frequencies [24], [32].…”
Section: Introductionmentioning
confidence: 99%
“…Another reason may be that those dispersive phenomena cannot follow the applied signal at high frequencies because of much longer de-trapping time constants (usually more than hundreds of microsecond) than the reciprocal of microwave frequencies [24], [32]. Furthermore, the published models [13], [28]- [31], [35] cannot be employed to model pulsed I-V curves with the current collapse critical point (CCCP) [30], [34], [36] in the pulsed I-Vcurves.…”
Section: Introductionmentioning
confidence: 99%
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