Analytical dVCE/dt Model of High-Power Trench Gate/Field-Stop IGBT Modules Considering Dynamical Conduction Current at Near-ZCT Transient

When high-power trench gate/field-stop insulated-gate bipolar transistor (Trench-FS IGBT) modules operate at near-zero current turn-off (near-ZCT), the conventional collector-emitter voltage rise slope ( dV_{\mathrm { CE}}/dt ) model does not consider the extension behavior of the space-charge regio...

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Veröffentlicht in:IEEE journal of emerging and selected topics in power electronics 2024-10, Vol.12 (5), p.4993-5003
Hauptverfasser: Li, Yue, Guo, Xizheng, Chen, Yueqing, Sun, Zonghui, You, Xiaojie
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container_title IEEE journal of emerging and selected topics in power electronics
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creator Li, Yue
Guo, Xizheng
Chen, Yueqing
Sun, Zonghui
You, Xiaojie
description When high-power trench gate/field-stop insulated-gate bipolar transistor (Trench-FS IGBT) modules operate at near-zero current turn-off (near-ZCT), the conventional collector-emitter voltage rise slope ( dV_{\mathrm { CE}}/dt ) model does not consider the extension behavior of the space-charge region (SCR) into the FS layer. In addition, it does not account for the effect of dynamic conduction current (DCC), resulting in poor model generality. To address these issues, this article first derives an expression for the voltage at the turning point where V_{\mathrm { CE}} exhibits a two-stage slope, occurring as the N-base region expands into the FS layer. Furthermore, the boundary conditions for V_{\mathrm { CE}} exhibiting a two-stage slope are determined. Second, based on the proposed expression and boundary conditions, accounting for the effect of DCC on the excess carrier concentration in the N-base region, a segmented analytical model for dV_{\mathrm { CE}}/dt is proposed. Finally, IGBT modules with various technologies and voltage ratings were experimentally tested. The results from simulations and hardware experiments validate the effectiveness and accuracy of the proposed method.
doi_str_mv 10.1109/JESTPE.2024.3444906
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In addition, it does not account for the effect of dynamic conduction current (DCC), resulting in poor model generality. To address these issues, this article first derives an expression for the voltage at the turning point where <inline-formula> <tex-math notation="LaTeX">V_{\mathrm { CE}} </tex-math></inline-formula> exhibits a two-stage slope, occurring as the N-base region expands into the FS layer. Furthermore, the boundary conditions for <inline-formula> <tex-math notation="LaTeX">V_{\mathrm { CE}} </tex-math></inline-formula> exhibiting a two-stage slope are determined. Second, based on the proposed expression and boundary conditions, accounting for the effect of DCC on the excess carrier concentration in the N-base region, a segmented analytical model for <inline-formula> <tex-math notation="LaTeX">dV_{\mathrm { CE}}/dt </tex-math></inline-formula> is proposed. Finally, IGBT modules with various technologies and voltage ratings were experimentally tested. 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In addition, it does not account for the effect of dynamic conduction current (DCC), resulting in poor model generality. To address these issues, this article first derives an expression for the voltage at the turning point where <inline-formula> <tex-math notation="LaTeX">V_{\mathrm { CE}} </tex-math></inline-formula> exhibits a two-stage slope, occurring as the N-base region expands into the FS layer. Furthermore, the boundary conditions for <inline-formula> <tex-math notation="LaTeX">V_{\mathrm { CE}} </tex-math></inline-formula> exhibiting a two-stage slope are determined. Second, based on the proposed expression and boundary conditions, accounting for the effect of DCC on the excess carrier concentration in the N-base region, a segmented analytical model for <inline-formula> <tex-math notation="LaTeX">dV_{\mathrm { CE}}/dt </tex-math></inline-formula> is proposed. Finally, IGBT modules with various technologies and voltage ratings were experimentally tested. 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In addition, it does not account for the effect of dynamic conduction current (DCC), resulting in poor model generality. To address these issues, this article first derives an expression for the voltage at the turning point where <inline-formula> <tex-math notation="LaTeX">V_{\mathrm { CE}} </tex-math></inline-formula> exhibits a two-stage slope, occurring as the N-base region expands into the FS layer. Furthermore, the boundary conditions for <inline-formula> <tex-math notation="LaTeX">V_{\mathrm { CE}} </tex-math></inline-formula> exhibiting a two-stage slope are determined. Second, based on the proposed expression and boundary conditions, accounting for the effect of DCC on the excess carrier concentration in the N-base region, a segmented analytical model for <inline-formula> <tex-math notation="LaTeX">dV_{\mathrm { CE}}/dt </tex-math></inline-formula> is proposed. Finally, IGBT modules with various technologies and voltage ratings were experimentally tested. 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subjects Analytical models
Boundary conditions
Capacitors
Carrier density
Collector-emitter voltage rise slope (dVCE/dt)
dynamic conduction current (DCC)
Electric potential
Emitters
Germanium
Insulated gate bipolar transistors
Logic gates
Modules
near-zero current turn-off (near-ZCT)
Semiconductor devices
space-charge region (SCR)
Transient analysis
trench gate/field-stop insulated-gate bipolar transistor (Trench-FS IGBT)
Voltage
title Analytical dVCE/dt Model of High-Power Trench Gate/Field-Stop IGBT Modules Considering Dynamical Conduction Current at Near-ZCT Transient
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