Titlebook: High-Brightness Accelerators; Anthony K. Hyder,M. Franklin Rose,Arthur H. Guenth Book 1988 Plenum Press, New York 1988 density.dynamics.el

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Wake Fields: Limitations and Possibilitiesept a portion of these fields and scatter them so that a second charge, following the first on the same path a distance s behind, will experience the scattered fields after the time it takes the speed of light to go from the scatterer to the axis of travel.

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Advanced Concepts for Acceleration speed that is a significant fraction of the speed of light. Both applications share the common goal of seeking to achieve accelerating gradients far in excess of those obtainable with conventional accelerating structures, e.g., E ≫ 10 MV/m.

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Injectors and Ion Sourcesnsport were very closely coupled. More recently the breakdown of the elements of an injector into separate components (see Fig. 1):.has lead progressively to optimization within each component and a fuller appreciation of the interactions between them.

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Radial Transmission-Line Linear Acceleratorsnge with currents less than 10 A (Fultz and Whitten, 1971). At the low end of the voltage range, the Phermex facility at Los Alamos Scientific Laboratories has been operated at 30 MeV and 500 A (Boyd et al., 1965; Moir et al., 1985).

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Introduction High-Brightness Acceleratorsneral applications. The range of accelerator designs and concepts reviewed varied from the TeV, low current devices to the multi-megampere, MeV accelerators used for the study of inertial confinement fusion. In almost all applications the beam brightness, the current per unit area per unit solid angle, plays an important role.

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