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Kim, K.-J.

  
Paper Title Page
WG341 Flat Electron Beams for a Smith-Purcell Backward Wave Oscillator for Intense Terahertz Radiation  
 
  • K.-J. Kim
    ANL, Argonne, Illinois
  • V. Kumar
    RRCAT, Indore (M. P.)
 
  A Smith-Purcell device can operate as a backward wave oscillator (BWO) producing a few watts of narrow bandwidth, CW Terahertz radiation. We discuss the requirements on electron beam properties for achieving the operation of such a device based on the results of a 2-D theory of Smith-Purcell BWO [1]. It is found that a specially designed non-relativistic electron beam is necessary with the current exceeding a certain threshold value and a flat transverse profile. Two methods for producing electron beams of required characteristics are discussed, one based on a line source and one employing the flat beam technique.

[1] V. Kumar and K.-J. Kim, Physical Review E 73, 026501 (2006).

 
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WG423 Transverse to Longitudinal Emittance Exchange to Improve Performance of High-Gain X-Ray Free Electron Laser  
 
  • K.-J. Kim
    ANL, Argonne, Illinois
  • P. Emma, Z. Huang
    SLAC, Menlo Park, California
  • P. Piot
    Northern Illinois University, DeKalb, Illinois
 
  The ability to generate small transverse emittance is a limiting factor for the performance of high-gain free electron lasers for X-rays. Noting that beams from an RF photocathode gun can have energy spread much smaller than that required for an X-ray FEL, we present a method to produce a normalized transverse emittance 0.1 mm·mrad, an order of magnitude smaller than the state-of-the-art. The method consists of producing a pancake-shaped beam of emittance (1, 1, 0.1) mm·mrad in the (x-,y-,z-)direction, applying the flat beam technique [1] to obtain (10, 0.1, 0.1) mm·mrad, and then exchanging the x-emittance with the longitudinal(z)-emittance, finally obtaining (0.1, 0.1, 10) mm·mrad. We show that the space charge effect does not degrade the small longitudinal emittance of the pancake-shaped beam. We found that the optical scheme studied previously [2] for an approximate longitudinal-transverse exchange is not adequate for the present case due to the large emittance ratio. However, we found a new scheme giving rise to an exact exchange necessary for the method. Results of preliminary simulation confirm the analytical theory.

[1] R. Brinkmann, Ya Derbenev, and K. Floettmann, Phys. Rev. ST Acc. Beams 4, 053501 (2001)

[2] M. Cornacchia and P. Emma, Phys. Rev. ST Acc. ST-AB 7 074401 (2004)

 
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