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Inverse Compton backscattering source driven by the multi-10 TW laser installed at Daresbury

  • G. Priebe
  • , D. Laundy
  • , M. A. MacDonald
  • , G. P. Diakun
  • , S. P. Jamison
  • , L. B. Jones
  • , D. J. Holder
  • , S. L. Smith
  • , P. J. Phillips
  • , B. D. Fell
  • , B. Sheehy
  • , N. Naumova
  • , I. V. Sokolov
  • , S. Ter-Avetisyan
  • , K. Spohr
  • , G. A. Krafft
  • , J. B. Rosenzweig
  • , U. Schramm
  • , F. Grüner
  • , G. J. Hirst
  • J. Collier, S. Chattopadhyay, E. A. Seddon
  • Daresbury Laboratory
  • Electronic Engineering and Physics Division
  • University of Dundee
  • Sheehy Scientific Consulting
  • University of Michigan
  • School of Mathematics and Physics
  • Queen's University of Belfast
  • Department of Electronic Engineering and Physics
  • University of the West of Scotland
  • Thomas Jefferson National Accelerator Facility
  • Department of Physics and Astronomy
  • University of California, Los Angeles
  • Institute of Radiooncology - OncoRay
  • Max-Planck Institut für Quantenoptik
  • CCLRC Rutherford Appleton Laboratory
  • Cockcroft Institute
  • Sci-Tech Daresbury

Research output: Contribution to journal › Article › peer-review

44 Citations (Scopus)

Abstract

Inverse Compton scattering is a promising method to implement a high brightness, ultra-short, energy tunable X-ray source at accelerator facilities. We have developed an inverse Compton backscattering X-ray source driven by the multi-10TW laser installed at Daresbury. Hard X-rays, with spectral peaks ranging from 15 to 30keV, depending on the scattering geometry, will be generated through the interaction of laser pulses with electron bunches delivered by the energy recovery linac machine, initially known as energy recovery linac prototype and subsequently renamed accelerators and lasers in combined experiments. X-ray pulses containing 9107 photons per pulse will be created from head-on collisions, with a pulse duration comparable to the incoming electron bunch length. For transverse collisions 8106 photons per pulse will be generated, where the laser pulse transit time defines the X-ray pulse duration. The peak spectral brightness is predicted to be ~1021photons/(smm2mrad20.1% /).

Original languageEnglish
Pages (from-to)649-660
Number of pages12
JournalLaser and Particle Beams
Volume26
Issue number4
DOIs
Publication statusPublished - 1 Dec 2008

Keywords

  • ALICE
  • Compton scattering
  • Compton synchrotron radiation
  • ERLP
  • Energy recovery linac
  • Laser Compton scattering
  • Laser synchrotron radiation
  • Thomson scattering
  • Ultra-short X-ray pulses
  • X-ray source

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