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Phys. Rev. E 68, 047401 (2003) [3 pages]

Plasma wakefield acceleration in self-ionized gas or plasmas

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S. Deng1, C. D. Barnes3, C. E. Clayton2, C. O’Connell3, F. J. Decker3, O. Erdem1, R. A. Fonseca2, C. Huang2, M. J. Hogan3, R. Iverson3, D. K. Johnson2, C. Joshi2, T. Katsouleas1, P. Krejcik3, W. Lu2, K. A. Marsh2, W. B. Mori2, P. Muggli1, and F. Tsung2
1University of Southern California, Los Angeles, California 90089, USA
2University of California, Los Angeles, California 90095, USA
3Stanford Linear Accelerator Center, Stanford, California 94309, USA

Received 8 April 2003; published 14 October 2003

Tunnel ionizing neutral gas with the self-field of a charged particle beam is explored as a possible way of creating plasma sources for a plasma wakefield accelerator [Bruhwiler et al., Phys. Plasmas (to be published)]. The optimal gas density for maximizing the plasma wakefield without preionized plasma is studied using the PIC simulation code OSIRIS [R. Hemker et al., in Proceeding of the Fifth IEEE Particle Accelerator Conference (IEEE, 1999), pp. 3672–3674]. To obtain wakefields comparable to the optimal preionized case, the gas density needs to be seven times higher than the plasma density in a typical preionized case. A physical explanation is given.

© 2003 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevE.68.047401
DOI:
10.1103/PhysRevE.68.047401
PACS:
52.25.Jm, 52.40.Mj