Abstract

The ability to generate small transverse emittance is perhaps the main limiting factor for the performance of high-gain x-ray free-electron lasers (FELs). Noting that beams from an rf photocathode gun can have energy spread much smaller than required for efficient FEL interaction, we present a method to produce normalized transverse emittance at or below about $0.1\text{ }\ensuremath{\mu}\mathrm{m}$, which will lead to a significantly shorter length undulator as well as a lower electron beam energy for an x-ray FEL project. The beam manipulation consists of producing an unequal partition of the initially equal emittances into two dissimilar emittances by a flat-beam technique and exchanging the larger transverse emittance with a smaller longitudinal emittance. We study various issues involved in the manipulation. In particular, a new emittance exchange optics we found enables an exact emittance exchange necessary for this scheme.

Highlights

  • Accelerated beams often need to be manipulated in phase space to optimize their efficiency for application

  • For a 1-A free-electron lasers (FELs) driven by a 15-GeV electron beam, the normalized emittance of the matched electron beam is about 0:2 m

  • We show that the manipulated beam improves the performance of x-ray FELs significantly

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Summary

INTRODUCTION

Accelerated beams often need to be manipulated in phase space to optimize their efficiency for application. With the typical rms bunch length of z 20 m (about 4 kA of peak current at a 1-nC bunch charge) and taking an increased energy spread of 1 10ÿ4 at 15 GeV, the normalized longitudinal emittance is about z 60 m This order-of-magnitude energy spread increase is necessary to suppress the microbunching instability associated with the bunch compression process

The scheme
Application for x-ray FELs
Space-charge effects on the gun emittances
The flat-beam technique
OPTICS FOR EMITTANCE EXCHANGE
SIMULATION STUDY
The injector
The emittance exchanger
Findings
FURTHER REMARKS AND CONCLUSIONS
Full Text
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