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Muggli, P.

Paper Title Page
MO2002 Energy Doubling in a Plasma Wakefield Accelerator 16
 
  • R. Ischebeck, M. K. Berry, I. Blumenfeld, F.-J. Decker, P. Emma, M. J. Hogan, R. H. Iverson, N. A. Kirby, P. Krejcik, R. Siemann, D. R. Walz
    SLAC, Menlo Park, California
  • C. E. Clayton, C. Huang, C. Joshi, W. Lu, K. A. Marsh, W. B. Mori, M. Zhou
    UCLA, Los Angeles, California
  • S. Deng, T. C. Katsouleas, P. Muggli, E. Oz
    USC, Los Angeles, California
 
  In the experiment E-167 at SLAC, the compressed electron pulse from the linac traverses a lithium vapor column and creates a plasma wake, which accelerates and focuses particles in the back of the pulse. Recent experimental results show that these fields can be sustained for 85 cm, increasing the particle energy from 42 GeV to 80 GeV. Plasma electrons can be trapped in the accelerating wake, resulting in ultra-short bunches with a relatively narrow energy spread and a small divergence angle. The results agree with three-dimensional particle-in-cell simulations.  
MOP026 Positron Source from X-rays Emitted by Plasma Betatron Motion 94
 
  • D. K. Johnson, C. E. Clayton, C. Huang, C. Joshi, W. Lu, K. A. Marsh, W. B. Mori, M. Zhou
    UCLA, Los Angeles, California
  • C. D. Barnes, I. Blumenfeld, F.-J. Decker, P. Emma, M. J. Hogan, R. Ischebeck, R. H. Iverson, N. A. Kirby, P. Krejcik, C. L. O'Connell, R. Siemann, D. R. Walz
    SLAC, Menlo Park, California
  • S. Deng, T. C. Katsouleas, P. Muggli, E. Oz
    USC, Los Angeles, California
 
  A new method for generating positrons has been proposed that uses betatron X-rays emitted by an electron beam in a high-K plasma wiggler. The plasma wiggler is an ion column produced by the head of the beam when the peak beam density exceeds the plasma density. The radial electric field of the beam blows out the plasma electrons transversely, creating an ion column. The focusing electric field of the ion column causes the beam electrons to execute betatron oscillations about the ion column axis. At the proper plasma density, this leads to synchrotron radiation in the 1-50 MeV range. These photons strike a thin (.5Xo), high-Z target and create electron-positron pairs. A computational model was written and matched with experimental results taken at the Stanford Linear Accelerator Center. This model was then used to design a more efficient positron source, giving positron yields of 0.44 positrons/electron, a number that is close to the target goal of 1-2 positrons/electron for future positron sources.