2018
DOI: 10.1364/oe.26.019318
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Annular beam driven high harmonic generation for high flux coherent XUV and soft X-ray radiation

Abstract: Separation of the high average power driving laser beam from the generated XUV to soft-X-ray radiation poses great challenges in collinear HHG setups due to the losses and the limited power handling capabilities of the typically used separating optics. This paper demonstrates the potential of driving HHG with annular beams, which allow for a straightforward and power scalable separation via a simple pinhole, resulting in a measured driving laser suppression of 5⋅10. The approach is characterized by an enormous… Show more

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Cited by 26 publications
(22 citation statements)
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“…In addition, the increased cutoff allows for > 1 mW of average power above 30 eV. Note, that for a high flux delivery, a gracing incidence plate [35] or annular beam driven HHG [36] in combination with a 100 nm aluminium filter could be used as a separator, resulting in an attenuation of the driving laser to < 1 μW with > 5 mW usable XUV average power on target. The Fourier-limited pulse duration of a single harmonic line corresponds to 3.4 fs pulse duration in the XUV (Fig.…”
Section: High Harmonic Generation Resultsmentioning
confidence: 99%
“…In addition, the increased cutoff allows for > 1 mW of average power above 30 eV. Note, that for a high flux delivery, a gracing incidence plate [35] or annular beam driven HHG [36] in combination with a 100 nm aluminium filter could be used as a separator, resulting in an attenuation of the driving laser to < 1 μW with > 5 mW usable XUV average power on target. The Fourier-limited pulse duration of a single harmonic line corresponds to 3.4 fs pulse duration in the XUV (Fig.…”
Section: High Harmonic Generation Resultsmentioning
confidence: 99%
“…This process can take place in every half cycle of the laser field, if the electric field is strong enough to free the electron. Nowadays, HHG is usually driven by state-of-the-art laser systems [6] in order to reach a higher flux of the emitted photons [7], a broader photon energy range of the generated harmonics [8], or to obtain an unprecedented time resolution of a few tens of attoseconds [9]; achievements which have already enabled numerous applications [10,11]. These characteristics are strongly influenced by the driving electric field, because strong-field electron dynamics is intricately linked with the time evolution of the driving laser.…”
Section: Introductionmentioning
confidence: 99%
“…However, with the increase of laser power, this portion will become stronger and it must be considered. In the high-repetition rate regime of ~100 kHz, several laboratories have used annular laser beams to generate high-order harmonics [27,70], while the measurement of the attosecond temporal duration was only reported in our previous work at ELI-ALPS [52].…”
Section: Generation Beam (Xuv Arm)mentioning
confidence: 99%
“…We make this distinction because temporal characterization is a demonstration of the attosecond pump-probe capability. As shown in Figure 1, single-pass HHG can provide high harmonics [17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36] up to tens of nJ per shot at 1 MHz by using powerful driving lasers with an average power up to ~100 W [37][38][39][40][41][42][43] and the attosecond pulses [44][45][46][47][48][49][50][51][52][53][54][55] up to hundreds of pJ per shot at 100 kHz. Intracavity HHG can deliver the high harmonics with the repetition rates up to hundreds of MHz [56][57][58][59][60][61][62][63].…”
Section: Introductionmentioning
confidence: 99%