Abstract

Electron beam energy chirp is an important parameter that affects the bandwidth and performance of a linac-based, free-electron laser. In this paper we study the wakefields generated by a beam passing between flat metallic plates with small corrugations, and then apply such a device as a passive dechirper for the Linac Coherent Light Source (LCLS) energy chirp control with a multi-GeV and femtosecond electron beam. Similar devices have been tested in several places at relatively low energies ($\ensuremath{\sim}100\text{ }\mathrm{MeV}$) and with relatively long bunches ($g1\text{ }\text{ }\mathrm{ps}$). In the parameter regime of the LCLS dechirper, with the corrugation size similar to the gap between the plates, the analytical solutions of the wakefields are no longer applicable, and we resort to a field matching program to obtain the wakes. Based on the numerical calculations, we fit the short-range, longitudinal wakes to simple formulas, valid over a large, useful parameter range. Finally, since the transverse wakefields---both dipole and quadrupole---are strong, we compute and include them in beam dynamics simulations to investigate the error tolerances when this device is introduced in the LCLS.

Highlights

  • In a linac-based X-ray free electron laser (FEL) there is often a need for energy chirp control of the beam as the magnetic compression employed in such FELs [1,2,3,4] typically leaves an undesired time-energy correlation in the bunch

  • In this paper we study the wakefields generated by a beam passing between flat metallic plates with small corrugations, and apply such a device as a passive dechirper for the Linac Coherent Light Source (LCLS) energy chirp control with a multi-GeV and femtosecond electron beam

  • We have investigated the use of a pair of flat metallic plates with small corrugations as a passive device for chirp control—a “dechirper”—a type of device that will be installed in the LCLS

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Summary

INTRODUCTION

In a linac-based X-ray free electron laser (FEL) there is often a need for energy chirp control of the beam as the magnetic compression employed in such FELs [1,2,3,4] typically leaves an undesired time-energy correlation in the bunch. While the chirp can be removed by off-crest acceleration in a following linac section, this solution can be costly or impractical, for a superconducting linac-based FEL For such cases, a dedicated passive structure that can intentionally generate a strong longitudinal wakefield was recently proposed to “dechirp” the beam. Fitting formulas of the longitudinal wakefield are obtained based on the field matching calculations, which are given in Appendix A The application of this structure to the LCLS of this structure is analyzed in Sec. III, including simulations of chirp control, the effects of the transverse wakefields and the subsequent tolerances for the beam position jitter and the misalignment of the structure necessary to preserve the transverse beam emittance.

Analytic formulas
Field matching method
Numerical results
Convergence studies
The wakefields
Higher band modes
APPLICATION TO LCLS CHIRP CONTROL
Dipole wakefield
Findings
CONCLUSIONS
Full Text
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