Fast Ionization-Front-Induced Anomalous Switching Behavior in Trigger Bipolar Transistors of Marx-Bank Circuits Under Base-Drive Conditions

The operation of transistorized Marx-bank circuits (MBCs) is analyzed, and physics-based modeling is used to understand the anomalous switching behavior of the first stage single trigger avalanche transistors of MBCs at high-current-injection conditions. The role of a voltage trigger pulse having variable rise time when applied to the base terminal is investigated to model the underlying physics of the anomalous switching behavior. Experimental observations related to ultrafast anomalous switching mechanisms of trigger transistor, i.e., either primary breakdown or current mode secondary breakdown, for faster and slower base drives are presented. This demonstrates the importance of the dynamic avalanche process and reverse saturation current on the switching mechanism under high-speed base-trigger ramps for different avalanche BJTs from various manufacturers and different lots. The agreement between 2-D TCAD device simulation results and the experimental observations shows the validity of the proposed theory when the base width and mobile carrier recombination rate are used as parameters in the device simulation setup.

[1]  A.F. Kardo-Sysoev,et al.  Fast power switches from picosecond to nanosecond time scale and their application to pulsed power , 1995, Digest of Technical Papers. Tenth IEEE International Pulsed Power Conference.

[2]  Kanad Mallik Nonuniform doping of the collector in avalanche transistors to improve the performance of Marx bank circuits , 2000 .

[3]  Y. Mizushima,et al.  New Instability Concept in Avalanche Diode Oscillation , 1974 .

[4]  R. J. Baker High voltage pulse generation using current mode second breakdown in a bipolar junction transistor , 1991 .

[5]  C. T. Kirk,et al.  A theory of transistor cutoff frequency (fT) falloff at high current densities , 1962, IRE Transactions on Electron Devices.

[6]  Amitabh Chatterjee Breakdown of transistors in Marx bank circuit , 2000 .

[7]  Chang Zenghu,et al.  High voltage fast ramp pulse generation using avalanche transistor , 1998 .

[8]  D. L. Scharfetter,et al.  Device physics of TRAPATT oscillators , 1970 .

[9]  P. L. Hower,et al.  Avalanche injection and second breakdown in transistors , 1970 .

[10]  Kanad Mallik The theory of operation of transistorized Marx bank circuits. , 1999 .

[11]  Kaustav Banerjee,et al.  Mechanisms leading to erratic snapback behavior in bipolar junction transistors with base emitter shorted , 2005 .

[12]  peixiong zhao,et al.  Modeling Erratic Behavior Due to High Current Filamentation in Bipolar Structures Under Dynamic Avalanche Conditions , 2016, IEEE Transactions on Electron Devices.

[13]  Amitabh Chatterjee,et al.  The principle of operation of the avalanche transistor-based Marx bank circuit: A new perspective. , 1998 .

[14]  Y. Mizushima,et al.  Properties of avalanche injection and its application to fast pulse generation and switching , 1967 .

[15]  H. Egawa,et al.  Avalanche characteristics and failure mechanism of high voltage diodes , 1966 .

[16]  W.P. Bennett,et al.  Power and energy limitations of bipolar transistors imposed by thermal-mode and current-mode second-breakdown mechanisms , 1981, IEEE Transactions on Electron Devices.

[17]  K. Ng,et al.  The Physics of Semiconductor Devices , 2019, Springer Proceedings in Physics.