2018
DOI: 10.1364/oe.26.016074
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10 W CEP-stable few-cycle source at 2 µm with 100 kHz repetition rate

Abstract: We developed a high repetition rate optical parametric chirped-pulse amplification (OPCPA) laser system based on fiber-laser-seeded Innoslab to generate few-cycle pulses around 2 µm with passively stable carrier-envelope phase (CEP) by difference frequency generation (DFG). Incorporating a piezo mirror before the DFG stage permits rapid CEP control. The OPCPA system is seeded by a stable supercontinuum generated in bulk material with the picosecond Innoslab pulses. Few-cycle pulses with durations of 17 fs and … Show more

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Cited by 55 publications
(18 citation statements)
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“…The standard deviation of the CEP as a function of accumulation time is then evaluated to be: 250 ± 60mrad, 310 ± 60mrad and 420 ± 50mrad for the 9sec, 90sec and 14min scans respectively. These values convey a reasonable CEP stability levels of the output, on par with the values commonly reported for OPA's and amplified lasers [14,[33][34][35][36][37]. Nevertheless, we believe that our hybrid amplifier has a capacity for a better CEP stability.…”
Section: Resultssupporting
confidence: 84%
“…The standard deviation of the CEP as a function of accumulation time is then evaluated to be: 250 ± 60mrad, 310 ± 60mrad and 420 ± 50mrad for the 9sec, 90sec and 14min scans respectively. These values convey a reasonable CEP stability levels of the output, on par with the values commonly reported for OPA's and amplified lasers [14,[33][34][35][36][37]. Nevertheless, we believe that our hybrid amplifier has a capacity for a better CEP stability.…”
Section: Resultssupporting
confidence: 84%
“…In this work, we report an OPA concept for producing an octave-spanning MIR spectrum and near-single-cycle pulses with high peak power and locked carrier-envelope phase while avoiding all of the above-mentioned problems. The work builds on our earlier reports about a related concept to generate CEP stable few cycle pulses in the 2 to 5 µm range [8,[26][27][28]. We combine a noncollinear OPA (NOPA) pumped by the second harmonic of a 1026 nm Yb:KGW-based pump laser with a collinear amplifier pumped by the residual fundamental pulses.…”
Section: Introductionmentioning
confidence: 99%
“…So far, accessing the SW-MIR wavelength region with watt-level average power and above was mostly achieved with complex parametric amplifiers, pumped by better established high-power systems in the 1 µm wavelength region [3,7]. However, this results in complex and inefficient systems.…”
Section: Introduction and State-of-the-artmentioning
confidence: 99%