• DocumentCode
    3211465
  • Title

    Plasma sources for future plasma wakefield accelerator based electron/positron collider

  • Author

    Muggli, P. ; Hogan, M.J. ; Seryi, A. ; Raubenheimer, T. ; Walz, D. ; Joshi, C. ; Katsouleas, T.C.

  • Author_Institution
    Electr. Eng.-Electrophyscis Dept., Univ. of Southern California, Los Angeles, CA, USA
  • fYear
    2009
  • fDate
    1-5 June 2009
  • Firstpage
    1
  • Lastpage
    1
  • Abstract
    Summary form only given. The recent experimental progress in plasma wakefield accelerator (PWFA) experiments make it possible to contemplate the application of the PWFA to a future electron positron linear collider. One of the main parameter of such a collider is the luminosity. The luminosity determines the number of occurrence of a given process with a given cross section, per unit time. For example, current designs call for luminosities in the 1034 cm-2s-1. To reach such luminosities, particle beams with average powers in the 10 MW range are necessary. In a plasma wakefield accelerator, a plasma works as an energy transformer to convert a relatively high-current, low-energy bunch train to a proportionately lower-current, higher-energy bunch train. This transformation is continued until the desired particle energy is reached to do physics. Microwave powered structures have a demonstrated ability to produce bunch trains with parameters of interest to the PWFA with high efficiency. Such structures operate most efficiently when the bunches are spaced tightly together, e.g. by a few ns. Consequently, the plasma source must be stable and reproducible on the ns time scale. Assuming an energy transfer efficiency from a PWFA drive bunch to the accelerated witness bunch of 35% implies that about 6.5 MW of beam power is left in the plasma. For a beam with an initial energy of 25 GeV, a final energy of 250 GeV and an accelerating gradient of 25 GeV/m, the total plasma length is 9 m, corresponding to an energy deposition of ap720 kW/m. The energy will be deposited in a very small volume of plasma, typically a radius of about 100 mum for densities of interest. Therefore, while heat evacuation at a large radius may not be a serious issue, thermal shock waves can be expected. These waves will modify the gas and plasma density for the following bunches. The beam and plasma source parameters will be presented, and the main issues with the plasma s- urce discussed.
  • Keywords
    colliding beam accelerators; electron-positron interactions; linear accelerators; plasma accelerators; plasma electromagnetic wave propagation; plasma sources; wakefield accelerators; PWFA based electron-positron linear collider; PWFA drive bunch; accelerated witness bunch; electron volt energy 25 GeV; electron volt energy 250 GeV; energy transfer efficiency; energy transformer; high current low energy bunch train transformation; low current high energy bunch train; luminosity; microwave powered structures; plasma sources; plasma wakefield accelerator; size 9 m; thermal shock waves; Acceleration; Electron accelerators; Linear accelerators; Particle beams; Plasma accelerators; Plasma applications; Plasma density; Plasma sources; Plasma waves; Positrons;
  • fLanguage
    English
  • Publisher
    ieee
  • Conference_Titel
    Plasma Science - Abstracts, 2009. ICOPS 2009. IEEE International Conference on
  • Conference_Location
    San Diego, CA
  • ISSN
    0730-9244
  • Print_ISBN
    978-1-4244-2617-1
  • Type

    conf

  • DOI
    10.1109/PLASMA.2009.5227314
  • Filename
    5227314