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Using a physicomathematical model, the process of current breaking in power semiconductor opening switches was investigated in p + - p - n - n + structures with different doping profiles. The model takes account of the actual doping profile of a structure, diffusion and drift of current carriers in a strong electric field, recombination via deep impurities and Auger recombination, and impact ionization in a dense plasma. The calculation of the electrical circuit of an opening switch is based on solution of Kirchhoff’s equations. It has been shown that in the nanosecond regime of breaking superhigh current densities with densities of the interrupted currents from a few to tens of kA/cm 2 , the dominant factor in the current breaking process is the width of the p -region in the initial doping profile of a structure. An increase in the p -region width from 100 to 200 µm makes the velocity of the excess plasma front propagating in the p -region in the reverse pumping stage higher by a factor of 5–7. Higher propagation velocity of the plasma front makes the current breaking process more intensive, which is manifested in the shorter current breaking time and higher overvoltage across the opening switch.
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Darznek et al. (2000) studied this question.
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