Computational Studies of Filamentary Pattern Formation in a High Power Microwave Breakdown Generated Air Plasma
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[1] Svilen Sabchevski,et al. The potential of the gyrotrons for development of the sub-terahertz and the terahertz frequency range — A review of novel and prospective applications , 2008 .
[2] C. Punset,et al. Self-organized filaments in dielectric barrier glow discharges , 1999 .
[3] G. Herring,et al. Microwave air breakdown enhanced with metallic initiators , 2008 .
[4] Allen Taflove,et al. Computational Electrodynamics the Finite-Difference Time-Domain Method , 1995 .
[5] A. D. Macdonald. Microwave breakdown in gases , 1966 .
[6] M. Shapiro,et al. Imaging of Atmospheric Air Breakdown Caused by a High-Power 110-GHz Pulsed Gaussian Beam , 2008, IEEE Transactions on Plasma Science.
[7] L. Pitchford,et al. Solving the Boltzmann equation to obtain electron transport coefficients and rate coefficients for fluid models , 2005 .
[8] R. Luebbers,et al. The Finite Difference Time Domain Method for Electromagnetics , 1993 .
[9] C. Postel,et al. Nanosecond Scale Discharge Dynamics in High Pressure Air , 2008, IEEE Transactions on Plasma Science.
[10] Jean-Pierre Boeuf,et al. Theory and modeling of self-organization and propagation of filamentary plasma arrays in microwave breakdown at atmospheric pressure. , 2010, Physical review letters.
[11] K. Yee. Numerical solution of initial boundary value problems involving maxwell's equations in isotropic media , 1966 .
[12] V. Bychkov,et al. Thermal ionization instability of an air discharge plasma in a microwave field , 2007 .
[13] A. Rousseau,et al. Patterns of Plasma Filaments Propagating on a Dielectric Surface , 2008, IEEE Transactions on Plasma Science.
[14] J. Boeuf,et al. Measurement and 3D simulation of self-organized filaments in a barrier discharge. , 2006, Physical review letters.
[15] John H. Booske,et al. Plasma physics and related challenges of millimeter-wave-to-terahertz and high power microwave generationa) , 2008 .
[16] L. Loeb,et al. The Mechanism of Spark Discharge in Air at Atmospheric Pressure. I , 1940 .
[17] G. Mur. Absorbing Boundary Conditions for the Finite-Difference Approximation of the Time-Domain Electromagnetic-Field Equations , 1981, IEEE Transactions on Electromagnetic Compatibility.
[18] Steven A. Cummer,et al. An analysis of new and existing FDTD methods for isotropic cold plasma and a method for improving their accuracy , 1997 .
[19] M. A. Shapiro,et al. Plasma structures observed in gas breakdown using a 1.5 MW, 110 GHz pulsed gyrotron , 2009 .
[20] S. G. Malyk,et al. A spherical plasmoid with a diffuse boundary in a linearly polarized quasistatic electromagnetic field , 2001 .
[21] Yoshiteru Hidaka,et al. Observation of large arrays of plasma filaments in air breakdown by 1.5-MW 110-GHz gyrotron pulses. , 2008, Physical review letters.
[22] D. Van Wie,et al. Surface Discharge in a Microwave Beam , 2007, IEEE Transactions on Plasma Science.
[23] V. Bityurin,et al. Electrodynamic model of a microwave streamer , 2009 .
[24] U. Ebert,et al. Positive Streamers in Ambient Air and a $\hbox{N}_{2}\!:\!\hbox{O}_{2}$ Mixture (99.8 : 0.2) , 2008, IEEE Transactions on Plasma Science.
[25] R. Cardoso,et al. Filamentation in argon microwave plasma at atmospheric pressure , 2009 .
[26] Willem Hundsdorfer,et al. An adaptive grid refinement strategy for the simulation of negative streamers , 2006, J. Comput. Phys..