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Phys. Rev. Lett. 97, 175003 (2006) [4 pages]

Positron Production by X Rays Emitted by Betatron Motion in a Plasma Wiggler

D. K. Johnson,1 D. Auerbach,1 I. Blumenfeld,2 C. D. Barnes,2 C. E. Clayton,1 F. J. Decker,2 S. Deng,3 P. Emma,2 M. J. Hogan,2 C. Huang,1 R. Ischebeck,2 R. Iverson,2 C. Joshi,1 T. C. Katsouleas,3 N. Kirby,2 P. Krejcik,2 W. Lu,1 K. A. Marsh,1 W. B. Mori,1 P. Muggli,3 C. L. O'Connell,2 E. Oz,3 R. H. Siemann,2 D. Walz,2 and M. Zhou1
1University of California, Los Angeles, California 90095, USA
2Stanford Linear Accelerator Center, Stanford, California 94309, USA
3University of Southern California, Los Angeles, California 90089, USA

Received 14 June 2006; published 27 October 2006

Positrons in the energy range of 3–30 MeV, produced by x rays emitted by betatron motion in a plasma wiggler of 28.5 GeV electrons from the SLAC accelerator, have been measured. The extremely high-strength plasma wiggler is an ion column induced by the electron beam as it propagates through and ionizes dense lithium vapor. X rays in the range of 1–50 MeV in a forward cone angle of 0.1 mrad collide with a 1.7 mm thick tungsten target to produce electron-positron pairs. The positron spectra are found to be strongly influenced by the plasma density and length as well as the electron bunch length. By characterizing the beam propagation in the ion column these influences are quantified and result in excellent agreement between the measured and calculated positron spectra.

©2006 The American Physical Society

URL: http://link.aps.org/doi/10.1103/PhysRevLett.97.175003
DOI: 10.1103/PhysRevLett.97.175003
PACS: 52.59.Ye; 41.75.Ht; 52.25.Jm; 52.40.Mj
  • 52.59.Ye
    Plasma devices for generation of coherent radiation
  • 41.75.Ht
    Relativistic electron and positron beams
  • 52.25.Jm
    Ionization of plasmas
  • 52.40.Mj
    Particle beam interactions in plasmas
  • YEAR: 2006

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