Abstract

The microbunching instability developed during the beam compression process in the linear accelerator (LINAC) of a free-electron laser (FEL) facility has always been a problem that degrades the lasing performance, and even no FEL is able to be produced if the beam quality is destroyed too much by the instability. A common way to suppress the microbunching instability is to introduce extra uncorrelated energy spread by the laser heater that heats the beam through the interaction between the electron and laser beam, as what has been successfully implemented in the Linac Coherent Light Source and Fermi@Elettra. In this paper, a simple and effective scheme is proposed to suppress the microbunching instability by adding two transverse gradient undulators (TGU) before and after the magnetic bunch compressor. The additional uncorrelated energy spread and the density mixing from the transverse spread brought up by the first TGU results in significant suppression of the instability. Meanwhile, the extra slice energy spread and the transverse emittance can also be effectively recovered by the second TGU. The magnitude of the suppression can be easily controlled by varying the strength of the magnetic fields of the TGUs. Theoretical analysis and numerical simulations demonstrate the capability of the proposed technique in the LINAC of an x-ray free-electron laser facility.

Highlights

  • X-ray free-electron lasers (FELs) hold great promise as ultrashort, tunable, intensity radiation sources for advanced user applications and open up new frontiers of ultrafast and ultrasmall sciences at the atomic scale

  • An X-band radio-frequency structure is employed before the first transverse gradient undulator (TGU) to compensate the second-order nonlinear components in the longitudinal phase space to avoid the undesired growth of transverse emittance and energy spread

  • The theoretical analysis shows that the TGU was able to suppress the instability by two factors: the additional slice energy spread and the longitudinal mixing from the transverse spread without changing the direction of the beam propagation

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Summary

Introduction

X-ray free-electron lasers (FELs) hold great promise as ultrashort, tunable, intensity radiation sources for advanced user applications and open up new frontiers of ultrafast and ultrasmall sciences at the atomic scale. In the x-ray FEL process, the required high intensity electron beams of subpicosecond (sub-ps) length are usually obtained by compressing longer beams in magnetic bunch compressors at relativistic energies.

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