Abstract

The presence of microbunching instabilities due to the compression of high-brightness electron beams at existing and future X-ray free-electron lasers (FELs) results in restrictions on the attainable lasing performance and renders beam imaging with optical transition radiation impossible. The instability can be suppressed by introducing additional energy spread, i.e., "heating" the electron beam, as demonstrated by the successful operation of the laser heater system at the Linac Coherent Light Source. The increased energy spread is typically tolerable for self-amplified spontaneous emission FELs but limits the effectiveness of advanced FEL schemes such as seeding. In this paper, we present a reversible electron beam heating system based on two transverse deflecting radio-frequency structures (TDSs) up and downstream of a magnetic bunch compressor chicane. The additional energy spread is introduced in the first TDS, which suppresses the microbunching instability, and then is eliminated in the second TDS. We show the feasibility of the microbunching gain suppression based on calculations and simulations including the effects of coherent synchrotron radiation. Acceptable electron beam and radio-frequency jitter are identified, and inherent options for diagnostics and on-line monitoring of the electron beam's longitudinal phase space are discussed.

Highlights

  • X-ray free-electron lasers (FELs) provide an outstanding tool for studying matter at ultrafast time and atomic length scales [1], and have become a reality with the operation of the Free-Electron Laser in Hamburg (FLASH) [2], the Linac Coherent Light Source (LCLS) [3], and the SPring-8 Angstrom Compact Free Electron Laser (SACLA) [4]

  • We present a reversible electron beam heating system based on two transverse deflecting radio-frequency structures (TDSs) upstream and downstream of a magnetic bunch compressor chicane

  • In order to suppress a microbunching instability associated with longitudinal bunch compression that deteriorates the FEL performance, the LCLS uses a laser heater system to irreversibly increase the uncorrelated energy spread within the electron bunches, i.e., the slice energy spread, to a level tolerable for operation of a self-amplified spontaneous emission FEL [8,9]

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Summary

INTRODUCTION

X-ray free-electron lasers (FELs) provide an outstanding tool for studying matter at ultrafast time and atomic length scales [1], and have become a reality with the operation of the Free-Electron Laser in Hamburg (FLASH) [2], the Linac Coherent Light Source (LCLS) [3], and the SPring-8 Angstrom Compact Free Electron Laser (SACLA) [4]. The required high transverse and longitudinal brightness of the x-ray FEL driving electron bunches may encounter various degradation effects due to collective effects like coherent synchrotron radiation (CSR) or microbunching instabilities In order to suppress a microbunching instability associated with longitudinal bunch compression that deteriorates the FEL performance, the LCLS uses a laser heater system to irreversibly increase the uncorrelated energy spread within the electron bunches, i.e., the slice energy spread, to a level tolerable for operation of a self-amplified spontaneous emission FEL [8,9]. The amount of tolerable beam heating is more restrictive and the longitudinal phase space control becomes more critical

METHOD
L yðsÞds
Linear beam optics
Matrix formalism
REVERSIBLE HEATING AND EMITTANCE PRESERVATION
A GHz MV MV m m
MICROBUNCHING GAIN SUPPRESSION
Analytical calculations
Numerical simulations
PRACTICAL CONSIDERATIONS
Jitter and tolerances
Integrated longitudinal phase space diagnostics
Findings
SUMMARY AND CONCLUSIONS
Full Text
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