Configuration schemes for nonadiabatic trapping of electrons in the nonlinear Interaction between an electron beam and two counterpropagating laser pulses

S. RUSCHIN; Z. SHEENA; A. GOVER; R. Z. OLSHAH; H. KLEINMAN

Conference on Lasers and Electro-Optics
OSA Technical Digest (Optica Publishing Group, 1988),
paper FA1

Configuration schemes for nonadiabatic trapping of electrons in the nonlinear Interaction between an electron beam and two counterpropagating laser pulses

S. RUSCHIN, Z. SHEENA, A. GOVER, R. Z. OLSHAH, and H. KLEINMAN

Conference on Lasers and Electro-Optics 1988

Anaheim, California United States
25–29 April 1988
ISBN: 1-55752-033-X

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Free-Electron Lasers (FA)

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S. RUSCHIN, Z. SHEENA, A. GOVER, R. Z. OLSHAH, and H. KLEINMAN, "Configuration schemes for nonadiabatic trapping of electrons in the nonlinear Interaction between an electron beam and two counterpropagating laser pulses," in Conference on Lasers and Electro-Optics, D. Pinnow and P. Moulton, eds., Vol. 7 of OSA Technical Digest (Optica Publishing Group, 1988), paper FA1.

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Abstract

Most efficiency enhancement schemes in free electron lasers are based on adiabatic changes in interaction parameters.¹ These changes (i.e., wiggler field period or Intensity changes) are slow enough to permit continuous power extraction from trapped electrons without changing the trapping fraction of the electrons. This fraction is, therefore, a very important parameter in the determination of the overall efficiency of the device. In most conventional amplifier schemes, trapping is determined by the Initial or injection conditions of the electron beam entering the interaction region.

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