Abstract

The energy modulation of 1.7-GeV electrons by femtosecond laser pulses was studied at the BESSY II ``femtoslicing'' source, a facility commissioned in 2004 for the purpose of producing sub-100 fs x-ray pulses. As a test case for future seeded free-electron lasers, the laser-electron interaction was investigated as function of various laser and electron beam parameters using different experimental methods.

Highlights

  • A laser pulse copropagating with an electron bunch in an undulator modulates the electron energy if the resonance condition L ˆ U 2 2 ‡ K2 2 (1)is fulfilled, i.e., if the laser wavelength L equals the wavelength of spontaneous undulator radiation

  • The oscillatory energy modulation has a period length equal to L and an envelope corresponding to the laser pulse shape enlarged by LNU, the distance by which electrons slip relative to the laser field over NU undulator periods

  • Laser-induced energy modulation has a number of promising applications, among them seeding schemes for free-electron lasers (FELs) such as high-gain harmonic generation (HGHG) [1], enhanced self-amplified spontaneous emission (ESASE) [2] or sideband seeding [3]

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Summary

INTRODUCTION

A laser pulse copropagating with an electron bunch in an undulator modulates the electron energy if the resonance condition. Laser-induced energy modulation has a number of promising applications, among them seeding schemes for free-electron lasers (FELs) such as high-gain harmonic generation (HGHG) [1], enhanced self-amplified spontaneous emission (ESASE) [2] or sideband seeding [3]. It is the basis of ‘‘femtoslicing,’’ a method to produce subpicosecond synchrotron radiation pulses in storage rings [4,5], and of schemes to generate subfemtosecond x-ray pulses in FELs [6 –8]. Femtoslicing serves as a test case for FEL seeding schemes, allowing to study the dependence of the energy modulation process on various parameters

The principle of femtoslicing and its implementation at BESSY
Relevant parameters
PREDICTION OF ENERGY MODULATION
Analytical estimate
Numerical simulation
Longitudinal electron distribution
Microbunching
Coherent THz radiation
Transverse electron distribution
Scraper measurements
Synchrotron radiation distribution
Other effects on the electron beam
Effect on the laser pulse
Findings
CONCLUSIONS
Full Text
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