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02 Figure 30- Coupling between center layer on stack 1 to center layer on stack 2 In the dielectric waif accelerator several conductors maybe located cm each dielectric layer leading to a configuration such as that shown in Figure 27. 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.

Blake, “Space-charge physics and the breakdown process; J. Appl. , 77, 2916 (1995). M. L. Kro~ D. Smitk D. N. E. J. Caporaso, P. Vitello, N. 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.

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.

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