By Peter E Abresch
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Rev. Lett. 61, 98 (1988) Accelerators," Sci. Am. 260, 54 (1989). , Laser Acceleration of Particles, AIP Conf. Proc. No. 130 (AIP, New York, 1985). 46R. J. Briggs, Phys. Rev. Lett. 54, 2588 (1985). This device falls into the category of wakefield 47W. accelerators. A. Barletta, Particle in Proceedings Acceleration Techniques, of the Workshop (CERN Service on New Developments d'Information, Orsay, in 1987), pp. 544-548. 48E. P. Lee, Livermore "Radiation National 49R. B. Palmer, edited - Laboratory New by S.
The beam velocity is Vb~C. 3) 9 charge, a is the beam radius, and H is the step function. The beam density on axis nb varies with s, on the time-scale l:r, the current rise time. As noted above, we assume throughout that current variation is adiabatic, ! Op'Cr > > 1 I, so that plasma oscillations a. MHD " equilibrium Equations. 4) are small in amplitude. With these assumptions, we calculate fields and plasma electron flow, using a cold fluid model. L,and t is time. The beam, electron Ph, Pe, and Pi and the beam and plasma electron potential.
Mizumachi, T. Ozaki and K. Takayama, Nucl. Inst'rum. Methods A285, 83 (1989). 5Use of ion-focussing and A. M. Sessler, Application International . Acceleration, to in a short-wavelength FEL is proposed in W. A. B_rletta High Gain, High Power Free-Electron TEV School Particle on Acceleration, Electromagnetic Proceedings Radiation and of the Particle INFN Beams edited by R. Bonifacio, L. De Salvo Souza, and C. Pellegrini (Elsevier Science Publishers B. , Amsterdam, 6For a discussion periodic Laser: Physics and variations of the transition in plasma 1988) pp.