The FERMI free-electron lasers

Allaria, E.; Badano, L.; Bassanese, S.; Capotondi, F.; Castronovo, D.; Cinquegrana, P.; Danailov, M.B.; D'Auria, G.; Demidovich, A.; De Monte, R.; De Ninno, G.; Di Mitri, S.; Diviacco, B.; Fawley, W.M.; Ferianis, M.; Ferrari, E.; Gaio, G.; Gauthier, D.; Giannessi, L.; Iazzourene, F.; Kurdi, G.; Mahne, N.; Nikolov, I.; Parmigiani, F.; Penco, G.; Raimondi, L.; Rebernik, P.; Rossi, F.; Roussel, E.; Scafuri, C.; Serpico, C.; Sigalotti, P.; Spezzani, C.; Svandrlik, M.; Svetina, C.; Trovó M.; Veronese, M.; Zangrando, D.; Zangrando, M.

doi:10.1107/S1600577515005366

Journal of Synchrotron Radiation Journal of
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Figure 6
(Left) Two-color FEL pulses, $[\lambda_{1}]$ and $[\lambda_{2}]$ , tuned across the Ti M-resonance, impinge on a Ti grating with a temporal separation Δt. (Right) Diffraction patterns corresponding to single-color `pump' and `probe' pulses and to two-color `pump'–`probe' pulses (delayed by 500 fs) for different flux (F) regimes: low-F = 10–30 mJ cm⁻², high-F = 2 J cm⁻².

JOURNAL OF
SYNCHROTRON
RADIATION

ISSN: 1600-5775

Volume 22| Part 3| May 2015| Pages 485-491

https://doi.org/10.1107/S1600577515005366

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