Abstract

We measured the interferences of the coherent radiation, produced by a train of electron bunches in an undulator and stored in an optical cavity. The device used here is a free-electron laser, whose optical cavity stores the radiation pulse for a multipass amplification process. The amplification process is avoided by detuning the optical cavity. This is done by increasing the cavity length, producing a desynchronism between the radiation pulses and electron bunches. Then, the output intensity is dependent on the cavity lengthening and exhibits periodical interferences. An analytical analysis makes a description of this effect. In practice, it allows a direct and simple measurement of the position of the ``zero detuning,'' corresponding to the perfect synchronism of the light pulse and electron bunch in the free-electron laser process.

Highlights

  • The CLIO facility is based on an infrared free-electron laser (FEL), provided to a large community of users [1,2,3]

  • We measured interference effects on the coherent radiation produced by the undulator of a free-electron laser below the laser threshold, using a detuning range of the optical cavity

  • This effect of interferences appears even if there is no amplification at all. It is due the superposition of the coherent emission pulses produced by the electron bunches in the undulator, which are stored in the optical cavity and are delayed along the round trips by length detuning

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Summary

INTRODUCTION

The CLIO facility is based on an infrared free-electron laser (FEL), provided to a large community of users [1,2,3] It uses an optical cavity with two mirrors, separated by a distance Lcav ≈ 4.8 m and adjusted to ensure synchronization between the laser and electron micropulses. The time structure of the CLIO accelerator is made of macropulses with a repetition rate of 25 Hz and a time duration of about 10 μs These include 600 micropulses separated by 16 ns, corresponding to 2.4 m, which is half of the cavity round-trip time; as a consequence, there are always two light pulses inside the optical cavity.

MEASUREMENT OF RADIATION AT VARIOUS CAVITY LENGTHS
MEASUREMENT OF RADIATION FOR VARIOUS UNDULATOR GAPS
THEORETICAL ANALYSIS
Resolution limit of oscillations
CONCLUSION
Summary of notation
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