Effect of random secondary delay times and emission velocities in electron multipactors

IEEE Transactions on Electron Devices

Volumn 44, Issue 3, 1997, Pages 489-497

  Riyopoulos, Spilios ^a   Chemin, David ^a   Dialetis, Demos ^a  

^a SCIENCE APPLICATIONS INTERNATIONAL CORPORATION   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

ELECTROMAGNETIC FIELDS; ELECTRON EMISSION; ELECTRON RESONANCE; ITERATIVE METHODS; QUENCHING;

ELECTRON IMPACT PHASE; ELECTRON MULTIPACTORS; EMISSION VELOCITY; RANDOM SECONDARY DELAY TIMES; SECONDARY EMISSION COEFFICIENT;

ELECTRON DEVICES;

EID: 0031104007     PISSN: 00189383     EISSN: None     Source Type: Journal    
DOI: 10.1109/16.556160     Document Type: Article

References (10)

1. P. T. Farnsworth, "Television by electron image scanning," J. Franklin Institute, vol. 218, pp. 411-444, 1934.
2. J. R. M. Vaughan, "Multipactor," IEEE Trans. Electron Devices, vol. 35, p. 1172, 1988.
3. _, "Observations of multipactor in magnetrons," IEEE Trans. Electron Devices, vol. ED-15, p. 883, 1968.
4. H. McDowell, "Multipactor discharge across a magnetic field," Varian interoffice mémo, 1976.
5. S. Riyopoulos, D. Chemin, and D. Dialetis, "Theory of electron multipactor in crossed-fields," Physics of Plasmas 2, p. 3194, 1995.
6. R. Kishek and Y. Y. Lau, "Interaction of multipactor discharge and rf circuit," Phys. Rev. Lett., vol. 75, p. 1218, 1995.
7. F. M. Mako, private communication 1996.
8. F. M. Mako and W. Peter, "A high-current micro-pulse electron gun," in Proc. 1993 IEEE Particle Accelerator Conf., p. 2702.
9. N/dX)/(dFN/dn+i); here X is any of the control variables ω, ε,u, T.
10. n+1)\ = |G| + 1 > 1. The map (8) must be iterated twice to ensure small relative changes in Ai/5 when -1 < G < 0. [11] For a discussion of Brownian motion/Langevin equation see R. Kubo, M. Toda, and N. Hasitsume in Statistical Physics II. Berlin: SpringerVelrag, 1978 pp. 1-39.