Monte Carlo modeling of secondary electron emission and its incorporation in particle simulations of electron-surface interaction

Abstract Based on Vaughanʼs empirical formula of secondary emission yield and the assumption of mutual exclusion of each type of secondary electron, a mathematically self-consistent secondary emission model is proposed. It identifies each generated secondary electron as either elastic reflected, rediffused, or true secondary, hence, it allows the use of distinct emission energy and angular distributions of each type of electron. Monte Carlo modeling of the developed model is presented, and second-order algorithms for particle collection and ejection at the secondary-emission wall are developed in order to incorporate the secondary electron emission process in the standard leap-frog integrator. The accuracy of these algorithms is analyzed for general fields and is confirmed by comparing the numerically computed values with the exact solution under a homogeneous magnetic field. In particular, the phenomenon of multipactor electron discharge on a dielectric is simulated to verify the usefulness of the model developed in this paper.

[1]  Robert J. Barker,et al.  High-power microwave sources and technologies , 2001 .

[2]  John P. Verboncoeur,et al.  Loading and injection of Maxwellian distributions in particle simulations , 2000 .

[3]  R. A. Kishek,et al.  MULTIPACTOR DISCHARGE ON A DIELECTRIC , 1998 .

[4]  M. Furman,et al.  Probabilistic Model for the Simulation of Secondary Electron Emission , 2002 .

[5]  J. Cazaux A new model of dependence of secondary electron emission yield on primary electron energy for application to polymers , 2005 .

[6]  C. Birdsall,et al.  Plasma Physics via Computer Simulation , 2018 .

[7]  G. Stupakov,et al.  Suppression of secondary emission in a magnetic field using triangular and rectangular surfaces , 2007 .

[8]  R. M. Vaughan,et al.  Secondary emission formulas , 1993 .

[9]  John P. Verboncoeur,et al.  Space-charge effects on multipactor on a dielectric , 2000 .

[10]  Algorithms for accurate relativistic particle injection , 2008, J. Comput. Phys..

[11]  Sang Ki Nam,et al.  Global Model for High Power Microwave Breakdown at High Pressure , 2008, 2008 IEEE International Power Modulators and High-Voltage Conference.

[12]  Hajo Bruining,et al.  Physics and applications of secondary electron emission , 1954 .

[13]  Lay Kee Ang,et al.  Power deposited on a dielectric by multipactor , 1998 .

[14]  Maheswaran Surendra,et al.  A Monte Carlo collision model for the particle-in-cell method: applications to argon and oxygen discharges , 1995 .

[15]  J. Verboncoeur Particle simulation of plasmas: review and advances , 2005 .

[16]  J. Vaughan,et al.  A new formula for secondary emission yield , 1989 .

[17]  A. Shih,et al.  Secondary emission properties as a function of the electron incidence angle , 1993 .

[18]  L. Lapierre,et al.  Multipactor discharge on a dielectric surface: Statistical theory and simulation results , 2005 .

[19]  John H. Booske,et al.  Plasma physics and related challenges of millimeter-wave-to-terahertz and high power microwave generationa) , 2008 .

[20]  John P. Verboncoeur,et al.  Multipactor electron discharge physics using an improved secondary emission model , 1998 .

[21]  J. Puech,et al.  Effect of emission velocity spread of secondary electrons in two-sided multipactor , 2005 .

[22]  Yang Feng,et al.  Algorithms for accurate collection, ejection, and loading in particle simulations , 2007, J. Comput. Phys..

[23]  A. Al-Bustani A new form of regenerative switching device-the camel switch , 1988 .

[24]  R. Lye,et al.  Theory of Secondary Emission , 1957 .