Abstract

In pulsed-beam free-electron devices, longitudinal space-charge fields result in collective effects leading to an expansion of short electron bunches along their trajectory. This effect restricts an application of intense ultrashort electron pulses in free-electron radiation sources. A careful theoretical treatment is required in order to achieve an accurate description of the self-fields and the resulted electron beam dynamics. In this paper, longitudinal space-charge fields are considered in the framework of a three-dimensional, space-frequency approach. The model is based on the expansion of the total electromagnetic field (including self-fields) in terms of transverse eigenmodes of the (cold) cavity, in which the field is excited and propagates. The electromagnetic field, originally obtained in the model as a solution of the wave equation, is shown to satisfy also Gauss's law. We applied the theory to derive an analytical expression for the longitudinal electric field of a pointlike charge, moving along a waveguide at a constant velocity. This enables consideration and study of the role played by different terms of the resulted expressions, such as components arising from forward and backward waves, propagating waves, and under cutoff frequencies, and so on. Possible simplifications in evaluation of longitudinal space-charge fields are discussed.

Highlights

  • Development of laser induced photocathodes and of electron bunch compression techniques enables application of intensive, ultrashort electron pulses in free-electron radiation sources

  • The electron beam is kept focused along the beam line so as the transverse components of the space-charge forces are compensated

  • The model is based on the expansion of the total electromagnetic field in terms of transverse eigenmodes of the cavity, in which the field is excited and propagates

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Summary

INTRODUCTION

Development of laser induced photocathodes and of electron bunch compression techniques enables application of intensive, ultrashort electron pulses in free-electron radiation sources. The model is based on the expansion of the total electromagnetic field in terms of transverse eigenmodes of the (cold) cavity, in which the field is excited and propagates. This approach has been applied for the analysis of wideband interactions in free-electron lasers operating in the linear and nonlinear regimes [7,8]. The longitudinal electric field was found in the model analytically for a pointlike charge, moving along a waveguide at a constant velocity This enables analysis of the role played by the different terms of the resulted expression for the longitudinal electric field, i.e., the components arising from forward and backward waves, above and under cutoff frequencies, and so on. Possible approximations for a simplified evaluation of longitudinal space-charge fields in a pulsed-beam device are discussed

MODAL PRESENTATION OF ELECTROMAGNETIC FIELD IN THE
Zq ZZ N q ZÃq
ONE-DIMENSIONAL LONGITUDINAL TERM
THE ELECTRON BEAM DYNAMICS
SINGLE CHARGE
STATIC POINTLIKE CHARGE IN A WAVEGUIDE
CONCLUSIONS
Methods
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