motion4 a n d controlling the t i m e d e p e n d e n t p a r a m e t e r s of t h e b e a m i n order t o optimize propagation of the b e a m i n full density air. R e s u l t s of experiments t o modify the b e a m p a r a m e t e r s a n d t h e i r effect of b e a m propagation i n full density a i r will be presented.
*Work sponsored by t h e Defense Advanced Research ProjectsAgency a n d the Office of N a v a l Research 'Sachs Freeman Associates, Landover, MD 20785 "SAIC, McLean, V A 22101 'E.P. L e e a n d R.K. Cooper, P a r t . Accel. '7,83 (1976).
ABSTRACTWe present here non-immersed apertured foilless diode designs developed for our Recirculating Linear Accelerator (RLA). They produce intense relativistic electron beams of low transverse velocities similar to those produced by our foil diode designs.' The anode foil is replaced by a four-range-thick anode plate with an aperture on axis. This configuration drastically increases the shot rate since there is no need for frequent foil changes and lengthy diode cavity pumpdowns. T h e performance of these diodes is currently being investigated with o u r low energy (1.5 MV) RLA injector and the 4-MV IBEX accelerator.A diode configuration with a large A-K gap (7 cm) and a very thin 6 mm in diameter cathode shank was investigated in detail. Particle and trajectory code simulations with only electrons are unable to reproduce the experimental results. It appears that the electron beam is focused by counterstreaming protons emitted from the anode aperture plate which intercepts the outer section of t h e e l e c t r o n beam. M A G I C simulations based on this assumption have reproduced quite well both the amplitude and the time evolution of the experimentally observed electron beams. A -600-A ion current can focus 15 k A of the electron heam throush the 3-cm anode aperture.presented and compared.A new high-gradient electron accelerator powered by modulated intense relativistic electron beams (MIREBs) has been developed at the Naval Research Laboratory. This accelerator is a combination of the two-beam and wake-field acceleration concepts. It relies on the interaction of two electron beams via a passive structure. The primary, or the driver beam is a large diameter MIREB, which transfers its RF power to a disk-loaded accelerating structure. The electromagnetic wave induced in this structure converges radially generating an average electric field of the order of 100 MV/m on the axis. A secondary electron beam is injected on the axis and accelerated by this hi h gradient field. electron beam emerged from a 1-m long accelerating structure, with a peak kinetic energy of 60 MeV and peak current of 200 Amperes. Simple scaling laws suggest that similar accelerators with much higher average electric fields can be built.In the experimentf,-a 0.2-cm-dia. secondary This work was supported by DOE, SDIO/HDL, and NRL. * TR ccllabcretic:: w i t ) . Y . Friezman, . I . P . 3 2 , 3 r d J. Krall. M . Friedman et al., Phys: Rev. Lett. a, 2468 (1989).A broadband (0.1-10 keV) conden...