scholarly journals Characterization of high-harmonic emission from ZnO up to 11  eV pumped with a Cr:ZnS high-repetition-rate source

2019 ◽  
Vol 44 (2) ◽  
pp. 259 ◽  
Author(s):  
Giulio Vampa ◽  
Sergey Vasilyev ◽  
Hanzhe Liu ◽  
Mike Mirov ◽  
Philip H. Bucksbaum ◽  
...  
2021 ◽  
Vol 11 (13) ◽  
pp. 6058
Author(s):  
Georgia Paraskaki ◽  
Sven Ackermann ◽  
Bart Faatz ◽  
Gianluca Geloni ◽  
Tino Lang ◽  
...  

Current FEL development efforts aim at improving the control of coherence at high repetition rate while keeping the wavelength tunability. Seeding schemes, like HGHG and EEHG, allow for the generation of fully coherent FEL pulses, but the powerful external seed laser required limits the repetition rate that can be achieved. In turn, this impacts the average brightness and the amount of statistics that experiments can do. In order to solve this issue, here we take a unique approach and discuss the use of one or more optical cavities to seed the electron bunches accelerated in a superconducting linac to modulate their energy. Like standard seeding schemes, the cavity is followed by a dispersive section, which manipulates the longitudinal phase space of the electron bunches, inducing longitudinal density modulations with high harmonic content that undergo the FEL process in an amplifier placed downstream. We will discuss technical requirements for implementing these setups and their operation range based on numerical simulations.


Instruments ◽  
2019 ◽  
Vol 3 (3) ◽  
pp. 47 ◽  
Author(s):  
Vittoria Petrillo ◽  
Michele Opromolla ◽  
Alberto Bacci ◽  
Illya Drebot ◽  
Giacomo Ghiringhelli ◽  
...  

Fine time-resolved analysis of matter—i.e., spectroscopy and photon scattering—in the linear response regime requires fs-scale pulsed, high repetition rate, fully coherent X-ray sources. A seeded Free Electron Laser (FEL) driven by a Linac based on Super Conducting cavities, generating 10 8 – 10 10 coherent photons at 2–5 keV with 0.2–1 MHz of repetition rate, can address this need. Three different seeding schemes, reaching the X-ray range, are described hereafter. The first two are multi-stage cascades upshifting the radiation frequency by a factor of 10–30 starting from a seed represented by a coherent flash of extreme ultraviolet light. This radiation can be provided either by the High Harmonic Generation of an optical laser or by an FEL Oscillator operating at 12–14 nm. The third scheme is a regenerative amplifier working with X-ray mirrors. The whole chain of the X-ray generation is here described by means of start-to-end simulations.


2016 ◽  
Vol 24 (16) ◽  
pp. 18133 ◽  
Author(s):  
Jan Rothhardt ◽  
Steffen Hädrich ◽  
Yariv Shamir ◽  
Maxim Tschnernajew ◽  
Robert Klas ◽  
...  

2012 ◽  
Vol 37 (23) ◽  
pp. 4892 ◽  
Author(s):  
Yoshitomo Okawachi ◽  
Reza Salem ◽  
Adrea R. Johnson ◽  
Kasturi Saha ◽  
Jacob S. Levy ◽  
...  

2021 ◽  
Vol 92 (10) ◽  
pp. 103203
Author(s):  
Patrik Straňák ◽  
Ludger Ploenes ◽  
Simon Hofsäss ◽  
Katrin Dulitz ◽  
Frank Stienkemeier ◽  
...  

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