Phys. Rev. ST Accel. Beams 3, 061301 (2000) [5 pages]

Dynamic effects in plasma wakefield excitation

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R. G. Hemker and W. B. Mori
Department of Physics and Astronomy, University of California at Los Angeles, Los Angeles, California 90095-1547

S. Lee and T. Katsouleas
Department of Electrical Engineering, University of Southern California, Los Angeles, California 90089-0271

Received 2 December 1999; published 26 June 2000

We have used 2D cylindrically symmetric particle-in-cell simulations to investigate the dynamics of a high energy electron beam propagating through an underdense plasma. The simulation parameters are relevant to a recent plasma wakefield experiment conducted at the Stanford Linear Accelerator Center [R. Assmann et al., Stanford Linear Accelerator Center Proposal, 1997]. We model the dynamic development of the beam and wakefield excitation over meters of propagation length. To most clearly illustrate the dynamics of both the beam and the wakefield, a video of the simulation data is presented. The main observation is that the beam dynamics, i.e., its betatron motion in the resulting ion channel, agree well with the theoretical predictions while the plasma wake remains almost invariant over the entire propagation distance. The video illustrates subtle details regarding the interplay between the beam dynamics and wakefield generation. The results presented here complement results published separately [S. Lee et al., Phys. Rev. E 61, 7014 (2000)].


©2000 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevSTAB.3.061301
DOI: 10.1103/PhysRevSTAB.3.061301
PACS: 52.65.Rr, 52.40.Mj, 41.75.-i

Supplemental Material

Video 1 [ RealMedia (244 kB) | GIF (4439 kB) | QuickTime (24916 kB) | AVI (19727 kB) ]
Thumbnail of Video 1 A video showing the parallel development of all the important properties of the beam and plasma as the system evolves in time. The different plots of the video are (column by column from the top to the bottom) Ez rubber sheet; Er-Bθ focusing field lineout σr off axis; Ez lineout on axis, beam-energy change as a function of z - ct; Er in the r - z plane; nbeam in the r - z; nplasma in the r - z plane (direction of r reversed). Please note that in the figures and the video the indices 1, 2, and 3 are used instead of z, r, and θ. The most important observation that can be made in this video is that the background plasma and the wakefield support change very little over time even though the beam changes strongly as it executes betatron oscillations and the beam tail gains energy.

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