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Temperature-Dependent Hot Electron Effects and Degradation Mechanisms in 650-V GaN-Based MIS-HEMT Power Devices Under Hard Switching Operations
22
Citations
26
References
2021
Year
Wide-bandgap Semiconductor650-V Gallium NitrideElectrical EngineeringEngineeringStress Test MethodPower DeviceApplied PhysicsPower Semiconductor DeviceHard Switching OperationsWide-bandgap SemiconductorsGan Power DeviceDegradation MechanismsElectric FieldPower ElectronicsMicroelectronicsSemiconductor Device
This article proposed a hard switching high-temperature reverse bias (HS-HTRB) stress test method with a high measurement delay tolerance to study the impacts and mechanisms of hot electron effects on the stability of threshold voltage ( <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$V_{\mathrm {th}}$ </tex-math></inline-formula> ) in 650-V gallium nitride (GaN)-based metal–insulator–semiconductor high-election mobility transistors (MIS-HEMTs). Conventional HTRB and high-temperature constant source current (HTSC) stress tests have been carried out as well. The electric field caused emission (or detrapping) of electrons in dielectrics results in a negative <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$V_{\mathrm {th}}$ </tex-math></inline-formula> shift, while buffer electron trapping leads to a positive <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$V_{\mathrm {th}}$ </tex-math></inline-formula> shift and degrades subthreshold slope. The hot current affects <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$V_{\mathrm {th}}$ </tex-math></inline-formula> in two different ways: channel impact ionization generates and accumulates holes under the gate and, thus, shifts <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$V_{\mathrm {th}}$ </tex-math></inline-formula> negatively by lowering the gate–source barrier, while injected hot electrons themselves shift <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$V_{\mathrm {th}}$ </tex-math></inline-formula> positively by depleting the channel electrons. As temperature rises, the intensity of impact ionization decreases while the hot electron injection strengthens. The appropriate level of hot current and substrate termination can help compensate the field-induced negative <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$V_{\mathrm {th}}$ </tex-math></inline-formula> shifts, ensuring a more stable working <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">$V_{\mathrm {th}}$ </tex-math></inline-formula> and, thus, a more reliable device for HS operations.
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