2021
DOI: 10.1063/5.0063225
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Synchronized beamline at FLASH2 based on high-order harmonic generation for two-color dynamics studies

Abstract: We present the design, integration, and operation of the novel vacuum ultraviolet (VUV) beamline installed at the free-electron laser (FEL) FLASH. The VUV source is based on high-order harmonic generation (HHG) in gas and is driven by an optical laser system synchronized with the timing structure of the FEL. Ultrashort pulses in the spectral range from 10 to 40 eV are coupled with the FEL in the beamline FL26, which features a reaction microscope (REMI) permanent endstation for time-resolved studies of ultrafa… Show more

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Cited by 4 publications
(3 citation statements)
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“…A first highharmonic source has recently been implemented at FLASH 2. 12 It is presently driven by the current OPCPA based laser.…”
Section: Discussionmentioning
confidence: 99%
“…A first highharmonic source has recently been implemented at FLASH 2. 12 It is presently driven by the current OPCPA based laser.…”
Section: Discussionmentioning
confidence: 99%
“…The REMI permanent end station, described in more detail in (50,54,55), has recently been upgraded by adding an absorption setup with an XUV spectrometer, which allows us to detect XUV spectra with a resolution of ~30 meV (56). In addition, a beamline for HHG driven by the output of the FLASH2 pump-probe OPCPA (optical parametric chirped-pulse amplification) laser system has been integrated into the FL26 beamline (57)(58)(59). By using the master timing system of the FLASH facility, the OPCPA system is synchronized with the FEL and produces the same pulse pattern.…”
Section: Methodsmentioning
confidence: 99%
“…The optical delay stage of the driving laser system can introduce up to 4 ns of time delay between the HHG and FEL pulses with femtosecond precision, allowing to study the dynamics of processes over a wide time range. After suppression of the remaining driving radiation by a 100-nm-thick Al filter, the HHG pulses are coupled into the FLASH2 beamline by means of a motorized hyperboloidal mirror, described in more detail in ( 57 , 58 ). From this point, the HHG beam propagates parallel to the FEL beam, shifted upward by around 7.5 mm.…”
Section: Methodsmentioning
confidence: 99%