Abstract

Influence of a linear energy chirp in the electron beam on a SASE FEL operation is studied analytically and numerically using 1-D model. Explicit expressions for Green's functions and for output power of a SASE FEL are obtained for high-gain linear regime in the limits of small and large energy chirp parameter. Saturation length and power versus energy chirp parameter are calculated numerically. It is shown that the effect of linear energy chirp on FEL gain is equivalent to the linear undulator tapering (or linear energy variation along the undulator). A consequence of this fact is a possibility to perfectly compensate FEL gain degradation, caused by the energy chirp, by means of the undulator tapering independently of the value of the energy chirp parameter. An application of this effect for generation of attosecond pulses from a hard X-ray FEL is proposed. Strong energy modulation within a short slice of an electron bunch is produced by few-cycle optical laser pulse in a short undulator, placed in front of the main undulator. Gain degradation within this slice is compensated by an appropriate undulator taper while the rest of the bunch suffers from this taper and does not lase. Three-dimensional simulations predict that short (200 attoseconds) high-power (up to 100 GW) pulses can be produced in Angstroem wavelength range with a high degree of contrast. A possibility to reduce pulse duration to sub-100 attosecond scale is discussed.

Highlights

  • Start-to-end simulations [1] of the TESLA Test FacilityFree Electron Laser (TTF FEL), Phase 1 [2], have shown the presence of a strong energy chirp within a short high-current leading peak in electron density distribution that has driven the self-amplified spontaneous emission (SASE) FEL process

  • According to the simulations, the energy chirp had a dramatic impact on SASE FEL saturation length and output characteristics

  • In this paper we study the impact of energy chirp on SASE FEL performance

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Summary

INTRODUCTION

Free Electron Laser (TTF FEL), Phase 1 [2], have shown the presence of a strong energy chirp (energy-time correlation) within a short high-current leading peak in electron density distribution that has driven the self-amplified spontaneous emission (SASE) FEL process. A similar effect takes place during the operation of VUV FEL at DESY in a ‘‘femtosecond mode’’ [3,4,5] Such a mode of operation might be possible in future x-ray SASE FELs. FELs (frequency chirp of SASE FEL radiation is correlated with energy chirp in the electron beam due to the FEL resonance condition) aiming at the shortening of radiation pulse with the help of a monochromator [6]. Reduced to the explicit expression in the limit of small energy chirp parameter up to the first order, resulting in phase correction (and ignoring the gain correction). This explicit solution for the Green’s function was used to analyze statistical properties of a chirped SASE FEL in this limit.

GREEN’S FUNCTION
A second-order expansion of the Green’s function takes the following form:
NONLINEAR REGIME
ENERGY CHIRP AND UNDULATOR TAPERING
GENERATION OF ATTOSECOND PULSES
BEYOND ‘‘FUNDAMENTAL LIMIT’’
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