2019
DOI: 10.1364/ol.44.005222
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Scalable 30  fs laser source with 530  W average power

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Cited by 44 publications
(28 citation statements)
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“…The experiment described in [17] can be interpreted similarly with a quasi-phase matching that is satisfied at 895 nm and 1235 nm, while the numerical simulation shows the initial appearance of sidebands at these wavelengths, with a progressive shift towards a greater wavelength separation from the pump upon propagation. We believe this shift to be due to the decrease of peak power caused by the non-negligible group-velocity dispersion of argon at a pressure of 4 bar.…”
Section: Quasi Phase Matched Four-wave Mixing In Mpcsmentioning
confidence: 74%
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“…The experiment described in [17] can be interpreted similarly with a quasi-phase matching that is satisfied at 895 nm and 1235 nm, while the numerical simulation shows the initial appearance of sidebands at these wavelengths, with a progressive shift towards a greater wavelength separation from the pump upon propagation. We believe this shift to be due to the decrease of peak power caused by the non-negligible group-velocity dispersion of argon at a pressure of 4 bar.…”
Section: Quasi Phase Matched Four-wave Mixing In Mpcsmentioning
confidence: 74%
“…In contrast, the modified 2D model proposed here typically takes a few tens of seconds to run on such a machine. The experiments are described in [16,17]. The model is implemented without any adjustable parameters based on the information provided in these references.…”
Section: Benchmarking Against Experimental Reportsmentioning
confidence: 99%
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“…This results in a record compression factor of ~32 at an excellent overall transmission of 95.7%. With this technique, the highest average power of 530 W was achieved compressing 590 fs 1.1 mJ pulses to 30 fs (20 times compression) at 500 kHz repetition rate in a 44-pass cell with a throughput of 96% [68].…”
Section: Multi-pass Cellsmentioning
confidence: 99%