Effect of RF Parameters on Breakdown Limits in High-Vacuum X-Band Structures
Author(s) -
Valery Dolgashev
Publication year - 2003
Publication title -
aip conference proceedings
Language(s) - English
Resource type - Conference proceedings
SCImago Journal Rank - 0.177
H-Index - 75
eISSN - 1551-7616
pISSN - 0094-243X
DOI - 10.1063/1.1635116
Subject(s) - rf power amplifier , radio frequency , hfss , limit (mathematics) , physics , linear particle accelerator , particle accelerator , pulsed power , power (physics) , pulse (music) , breakdown voltage , computational physics , optics , materials science , electrical engineering , optoelectronics , engineering , beam (structure) , voltage , amplifier , antenna (radio) , mathematical analysis , microstrip antenna , mathematics , cmos , quantum mechanics , detector
RF breakdown is one of the major factors determining performance of high power rf components and rf sources. RF breakdown limits working power and produces irre- versible surface damage. The breakdown limit depends on the rf circuit, structure geom- etry, and rf frequency. It is also a function of the input power, pulse width, and surface electric and magnetic fields. In this paper we discuss multi-megawatt operation of X- band rf structures at pulse width on the order of one microsecond. These structures are used in rf systems of high gradient accelerators. Recent experiments at Stanford Linear Accelerator Center (SLAC) have explored the functional dependence of breakdown limit on input power and pulse width. The experimental data covered accelerating structures and waveguides. Another breakdown limit of accelerating structures was associated with high magnetic fields found in waveguide-to-structure couplers. To understand and quan- tify these limits we simulated 3D structures with the electrodynamics code Ansoft HFSS and the Particle-In-Cell code MAGIC3D. Results of these simulations together with ex- perimental data will be discussed in this paper.
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