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Two-color dual-oscillator infrared free-electron laser

Wieland Schöllkopf*, Sandy Gewinner, Marco De Pas, Heinz Junkes, Sebastian Kray, William Kirstaedter, William B. Colson†, David H. Dowell†, Stephen C. Gottschalk† et al.

John W. Rathke†, Tom J. Schultheiss†, Alan M. M. Todd†, Lloyd M. Young†, Akash Chandra Behera, América Y. Torres-Boy, Martin Wolf, Alexander Paarmann, Gert von Helden, and Gerard Meijer

  • *Contact author: wschoell@fhi-berlin.mpg.de
  • †Consultant to the Fritz-Haber-Institut der Max-Planck-Gesellschaft, Faradayweg 4-6, 14195 Berlin, Germany.

Phys. Rev. Accel. Beams 29, 103403 – Published 13 October, 2026

DOI: https://doi.org/10.1103/b27b-9gg1

Abstract

We report on the design and performance of a two-color dual-oscillator infrared free-electron laser (FEL). The midinfrared (MIR) FEL at the Fritz Haber Institute has been upgraded to include a second oscillator FEL beamline that permits lasing in the far-infrared (FIR) regime from 4.5 to 175  μm. In addition, a 500 MHz kicker cavity has been installed downstream of the electron accelerator. It allows deflection of electron bunches of up to 50 MeV energy alternately left and right by an angle of ±2°. It can, thus, split the high-repetition rate (1 GHz) electron bunch train from the accelerator into two bunch trains of 500 MHz repetition rate each; one is steered to the MIR FEL and the other one to the new FIR FEL. In this two-color mode of simultaneous, synchronized operation, the wavelengths in both FELs can be tuned independently over wide ranges of up to a factor of 4 each by undulator gap variation. In addition, two-color operation is also available at reduced repetition rates (e.g., 55.6 MHz of both MIR and FIR pulses), as needed for some applications. This unique two-color mode opens up a wealth of novel user applications, such as MIR-FIR pump-probe experiments.

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