Cathode Priming vs. RF Priming for Relativistic Magnetrons

POSTER

Abstract

Magnetron start-oscillation time, pulsewidth and pi-mode locking are experimentally compared for RF priming versus cathode priming on the Michigan-Titan relativistic magnetron (-300 kV, 2-10 kA, 300-500 ns). Cathode priming [1, 2] is an innovative technique first demonstrated experimentally at UM. In this technique, the cathode is fabricated with N/2 emitting strips or N/2-separate cathodes (for an N-cavity magnetron), which generate the desired number of spokes for pi-mode. Cathode priming yields 13{\%} faster startup with more reproducible pi-mode oscillation. Radio Frequency (RF) priming is investigated as the baseline priming technique for magnetrons. The external priming source is a 100kW, 3\textbf{$\mu $}s pulsewidth magnetron on loan from AFRL. RF priming reduced startup delay by 15{\%} and increased pulsewidth by 9{\%}. [1] M.C. Jones, V.B. Neculaes, R.M. Gilgenbach, W.M. White, M.R. Lopez, Y.Y. Lau, T.A. Spencer, and D. Price, Rev. Sci. Inst., 75, 2976 (2004) [2] M.C. Jones, Doctoral Dissertation, University of Michigan, 2005

*Research supported by AFOSR and AFRL

Authors

  • W.M. White

  • B.W. Hoff

  • R.M. Gilgenbach

  • Y.Y. Lau

  • M.C. Jones

  • V.B. Neculaes

  • N. Jordan

  • P. Pengvanich

  • R. Edgar

    • Intense Energy Beam Interaction Lab, Nuclear Engineering \& Radiological Sciences Dept., University of Michigan, Ann Arbor, MI 48109
  • T.A. Spencer

    • Air Force Research Lab, Kirtland AFB, NM
  • D. Price

    • Titan Corp., San Leandro, CA