31st European Solid-State Device Research Conference 2001
DOI: 10.1109/essderc.2001.195205
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Compensation devices versus power MOS and high speed IGBT - a device physics based guideline for the application

Abstract: This article focuses on the advantages and technological challenges of state-ofthe-art power devices for fast switching applications. It covers the power MOSFET, the high speed IGBT and the recently introduced compensation devices with 600 V blocking capability. Special emphasis is laid on the charge compensation principle.The device physics of all concepts are discussed in detail with respect to different operating conditions. The special requirements of compensation devices as well as todays and conceiveable… Show more

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Cited by 9 publications
(2 citation statements)
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“…The breakdown voltage of the CoolMOS is a quantity that very sensitively reacts to any additional charge which disturbs the exact charge balance between n and p columns in the blocking state, because even a slight charge imbalance causes the electric field distribution to change from trapezoidal to triangular shape leading to a drastic reduction of the blocking voltage BV DSS . 22 Figure 13 shows that BV DSS progressively degrades with increasing fluence of electron irradiation for the lower annealing temperature at T ϭ 493 K, but fully recovers to the initial value of the nonirradiated device for an annealing temperature of T ϭ 623 K. Under the assumption that the defects may induce a homogeneous change of the n or the p doping, simulations of the breakdown voltage reproduce the experimental data with a value of the additional p doping slightly higher than the n doping ͑Fig. 13͒.…”
Section: Optimization Of the Coolmos™ Body Diodementioning
confidence: 99%
“…The breakdown voltage of the CoolMOS is a quantity that very sensitively reacts to any additional charge which disturbs the exact charge balance between n and p columns in the blocking state, because even a slight charge imbalance causes the electric field distribution to change from trapezoidal to triangular shape leading to a drastic reduction of the blocking voltage BV DSS . 22 Figure 13 shows that BV DSS progressively degrades with increasing fluence of electron irradiation for the lower annealing temperature at T ϭ 493 K, but fully recovers to the initial value of the nonirradiated device for an annealing temperature of T ϭ 623 K. Under the assumption that the defects may induce a homogeneous change of the n or the p doping, simulations of the breakdown voltage reproduce the experimental data with a value of the additional p doping slightly higher than the n doping ͑Fig. 13͒.…”
Section: Optimization Of the Coolmos™ Body Diodementioning
confidence: 99%
“…The fabrication of mostly charge compensated n-and p-pillars is hence the key to enabling this technology. Detailed information on the device physics, implementation issues, and behavior of SJ devices can be found in [14]- [16]. In Fig.…”
Section: Switching Model Of a Power Mosfetmentioning
confidence: 99%