Surface recombination in breakdown time delay experiments: Effect of different cathode materials

1996 ◽  
Vol 16 (2) ◽  
pp. 195-208 ◽  
Author(s):  
V. Lj. Marković ◽  
M. M. Pejović ◽  
Z. Lj. Petrović
Keyword(s):  
Time Delay ◽  
Cathode Materials ◽  
Surface Recombination ◽  
Breakdown Time

Experimental Study on Breakdown Time Delay of Hundreds of Nanoseconds Pulse Under Different du/dt for mm Gaps

2019 ◽  
Vol 47 (10) ◽  
pp. 4579-4583 ◽  
Author(s):  
Fan Guo ◽  
Shi He ◽  
Wei Jia ◽  
Junna Li ◽  
Zhiqiang Chen ◽  
...  
Keyword(s):  
Experimental Study ◽  
Time Delay ◽  
Breakdown Time

Statistical analysis of the electrical breakdown time delay distributions in krypton

2006 ◽  
Vol 13 (8) ◽  
pp. 083502 ◽  
Author(s):  
Čedomir A. Maluckov ◽  
Jugoslav P. Karamarković ◽  
Miodrag K. Radović ◽  
Momčilo M. Pejović
Keyword(s):  
Statistical Analysis ◽  
Time Delay ◽  
Electrical Breakdown ◽  
Breakdown Time

The application of convolution-based statistical model on the electrical breakdown time delay distributions in neon

2004 ◽  
Vol 11 (11) ◽  
pp. 5328-5334 ◽  
Author(s):  
Čedomir A. Maluckov ◽  
Jugoslav P. Karamarković ◽  
Miodrag K. Radović ◽  
Momčilo M. Pejović
Keyword(s):  
Time Delay ◽  
Statistical Model ◽  
Electrical Breakdown ◽  
Breakdown Time

scholarly journals Homogeneous gas phase models of relaxation kinetics in neon afterglow

2007 ◽  
Vol 5 (1) ◽  
pp. 33-44 ◽  
Author(s):  
Vidosav Markovic ◽  
Sasa Gocic ◽  
Suzana Stamenkovic
Keyword(s):  
Experimental Data ◽  
Time Delay ◽  
Gas Phase ◽  
Number Density ◽  
Relaxation Kinetics ◽  
Particle Decay ◽  
Breakdown Time ◽  
Active Particles ◽  
Effective Coefficients ◽  
Phase Models

The homogeneous gas phase models of relaxation kinetics (application of the gas phase effective coefficients to represent surface losses) are applied for the study of charged and neutral active particles decay in neon afterglow. The experimental data obtained by the breakdown time delay measurements as a function of the relaxation time td (?) (memory curve) is modeled in early, as well as in late afterglow. The number density decay of metastable states can explain neither the early, nor the late afterglow kinetics (memory effect), because their effective lifetimes are of the order of milliseconds and are determined by numerous collision quenching processes. The afterglow kinetics up to hundreds of milliseconds is dominated by the decay of molecular neon Ne2 + and nitrogen ions N2 + (present as impurities) and the approximate value of N2 + ambipolar diffusion coefficient is determined. After the charged particle decay, the secondary emitted electrons from the surface catalyzed excitation of nitrogen atoms on the cathode determine the breakdown time delay down to the cosmic rays and natural radioactivity level. Due to the neglecting of number density spatial profiles, the homogeneous gas phase models give only the approximate values of the corresponding coefficients, but reproduce correctly other characteristics of afterglow kinetics from simple fits to the experimental data.

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