Abstract

We present the experimental demonstration of a method for generating two spectrally and temporally separated pulses by an externally seeded, single-pass free-electron laser operating in the extreme-ultraviolet spectral range. Our results, collected on the FERMI@Elettra facility and confirmed by numerical simulations, demonstrate the possibility of controlling both the spectral and temporal features of the generated pulses. A free-electron laser operated in this mode becomes a suitable light source for jitter-free, two-colour pump-probe experiments.

Highlights

  • Chirped pulse modulation is a widely used technique, with relevant applications in several fields of research, ranging from digital communication [1] to radar detection [2], and from optics [3] to laser physics

  • The paper is divided into the following parts: in Section 1 we introduce the principle upon which a coherent harmonic generation (CHG) free-electron laser (FEL) is based, with specific reference to the case of the FERMI@Elettra FEL [17]

  • As we remarked in the previous section, a linear energy chirp of the electron energy induces a spectral shift of the FEL emission

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Summary

Introduction

Chirped pulse modulation is a widely used technique, with relevant applications in several fields of research, ranging from digital communication [1] to radar detection [2], and from optics [3] to laser physics. Frequency chirping is employed to stretch a short pulse prior to amplification. We characterize the performance of a seeded FEL where frequency chirping on the seed laser is instead exploited to generate two independent pulses spectrally and temporally separated in an externally controllable fashion. At FERMI@Elettra, multiple pulses have been obtained recently with a different technique, based on the simultaneous injection of two different seed pulses on the same electron bunch [11]. In this case the two pulses minimum separation is limited by the seed pulse length. We summarize our conclusions and provide some perspectives for future experimental studies

Formation of the spectral double peak
Experimental results
Simulations
Conclusion
Full Text
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