2014
DOI: 10.3390/photonics1040442
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Grating Configurations for the Spectral Selection of Coherent Ultrashort Pulses in the Extreme-Ultraviolet

Abstract: Abstract:The design and realization of grating instruments to handle and condition coherent ultrafast pulses in the extreme ultraviolet spectral region are discussed. The main application of such instruments is the spectral selection of high-order laser harmonics and free-electron-laser pulses in the femtosecond time scale. Broad-band monochromators require the use of diffraction gratings at grazing incidence. Here, we discuss two configurations useful for the realization of grating monochromator with ultrafas… Show more

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Cited by 7 publications
(9 citation statements)
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References 32 publications
(31 reference statements)
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“…a) Cluster source, Naoven chamber, and photoelectron/mass spectrometer. b) UV and EUV laser light source with high harmonic generation (HHG) and HH monochromator 51,52 . BS: beam splitter, / 2  : half-wave plate, L: focusing lens, GC: gas cell, TM1, TM2 and TM3: toroidal mirrors, q in /q out : input/output arms, G: grating,  : altitude angle, S: exit slit.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…a) Cluster source, Naoven chamber, and photoelectron/mass spectrometer. b) UV and EUV laser light source with high harmonic generation (HHG) and HH monochromator 51,52 . BS: beam splitter, / 2  : half-wave plate, L: focusing lens, GC: gas cell, TM1, TM2 and TM3: toroidal mirrors, q in /q out : input/output arms, G: grating,  : altitude angle, S: exit slit.…”
Section: Methodsmentioning
confidence: 99%
“…1b). A home-built time-preserving monochromator in the off-plane mount geometry following the design by Poletto and coworkers 51,52 was used for the spectral selection of the HHs. Depending on the operation parameters, the monochromator provides photon fluxes between 10 8 and 10 11 photons/s at the output with EUV pulse durations between 50fs and 80fs 55 .…”
Section: Methodsmentioning
confidence: 99%
“…After di raction at the grating, the light is focused by T3 into the exit plane, where a slit de nes the energy resolution. For the use of the fs XUV pulses in time resolving experiments, we make use of a special monochromator geometry to minimize pulse broadening e ects (Fabio Frassetto & Poletto, 2014). Passing through a grating monochromator a ects the pulse length in two ways: (1) the monochromator acts as a frequency bandpass with a nite bandwidth.…”
Section: Beamlinementioning
confidence: 99%
“…(2) the di raction at a grating adds a geometric broadening of the pulse time pro le due to di erent optical pathlenths. We adopt the design described in (Fabio Frassetto & Poletto, 2014) as o -plane-mounting, which minimizes the second e ect by orienting the gratings grooves along the light incidence direction. To minimize the rst e ect, we design the monochromator to have an energy resolution that is just su cient to separate adjacent harmonic lines.…”
Section: Beamlinementioning
confidence: 99%
“…The new rotation scheme enables the construction of such a monochromator using only two plane grating reflections, eliminating the need for the additional two concave mirrors employed with current state-of-the-art time-compensated monochromators [18].…”
Section: A Two-element Time-compensated Monochromatormentioning
confidence: 99%