Interaction of multipactor and RF circuit

Proceedings of SPIE - The International Society for Optical Engineering

Volumn 2843, Issue , 1996, Pages 160-165

  Kishek, R ^a   Lau, Y Y ^a   Chernin, D ^b   Gilgenbach, R M ^a  

^a UNIVERSITY OF MICHIGAN   (United States)

^b SCIENCE APPLICATIONS INTERNATIONAL CORPORATION   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

ELECTRONS; TIMING CIRCUITS;

ELECTRON IMPACT ENERGY; FOCUSING MECHANISMS; MULTIPACTOR DISCHARGE; MUTUAL REPULSION; SECONDARY ELECTRON YIELD; SIMPLE MODELING; SPACE CHARGE FORCES; TEMPORAL EVOLUTION;

ELECTRIC DISCHARGES;

EID: 85075916946     PISSN: 0277786X     EISSN: 1996756X     Source Type: Conference Proceeding    
DOI: 10.1117/12.255408     Document Type: Conference Paper

References (6)

1. J. R. M. Vaughan, IEEE Trans. ED-35, 1 172 (1988).
2. S. Riyopoulos, D. Chemin, and D. Dialetis, Phys. Plasmas 2, 3194 (1995).
3. R. Kishek and Y. Y. Lau, Phys. Rev. Lett. 75, 1218 (1995).
4. R. Kishek and Y. Y. Lau, Phys. Plasmas 3, 148 1 (1996).
5. It is shown by Riyopoulos et al [Ref. 2] that the inclusion of the initial velocity of the secondary electrons does not qualitatively change their steady state solutions.
6. if the impact energy E is greater (less) than the first cross-over point E1, more (fewer) electrons will be released by secondary emission. As a result, more (less) energy will be drained from the cavity as it accelerates more (fewer) secondary