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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. As can be seem in Figures 28-30 adding adjacent stacks in close proximity to each other can significantly increase the mutual coupling between transmission lines.

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.

This technology is potentially an ultra compact accekrator/pulsed power driver. This new accelerator relies on three new components an ultra-high gradient insulator, an asymmetric Blumle@ and low jitter switches. In this repo~ we fmsed our attention on the first two components of the DWA system: the insulators and the asymmetric Bhunlein. First, we sought to develop the necessq design tools to model and scale the behavior of the high gradient insulator. , initiation and creation of the surface discharge).

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Advanced Accelerator Theory Development


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