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Tishchenko, “Vacuum Surface Flashover and High Pressure Gas Streamers: (1997). L. , “Measured and Theoretical Characterization of the RF Properties of Stacked, H@-Gradknt Insulator Material” Proceedings of the 1997 IEEE Particle Accelerator Conf’ence, Vancouver, BC, Cana~ 12–16 May 1997. [12] S. L. , “Longitudinal Impedance Measurements of an RK-TBA kduction Accelerating Gap” Proceedings of the 1997 IEEE Particle Accelerator Conference, Vancouver, BC, Canad~ 12–16 May 1997.

That is, the tip of a propagating streamer is known to produce intense high energy radiation emission which we believe can lead to photoconduction in the insulator. As conduction in the insulator will strongly modfi the voltage which drives the streamer discharge, accurate coupling of the streamer to the insulator were included. We showed initial calculations that were pdormed. The electromagnetic characteristics of the HGI are due to perturbing the geometry of the resonant cavity. Carefil incorporation of HGI’s into an induction cell design should always lead to a much lower impedance than that of a conventional solid insulator.

In this geometry if the gap between adjacent layers is sufficiently close the mutual coupling between transmission lines can be substantially increased. In this case we still drive the center transmission line (line number 10) on stack number 1 and determine the cuupling coefficients to the other transmission lines. The pa-28- rameters associated with the individual stacks are the same as before. 5 mm. Figures 28 and 29 show the electric and magnetic coupling into stack 2 with the center transmission line driven in stack 1.