2014
DOI: 10.1364/ol.39.001422
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Power scaling of supercontinuum seeded megahertz-repetition rate optical parametric chirped pulse amplifiers

Abstract: Optical parametric chirped-pulse amplifiers with high average power are possible with novel high-power Yb:YAG amplifiers with kW-level output powers. We demonstrate a compact wavelength-tunable sub-30-fs amplifier with 11.4 W average power with 20.7% pump-to-signal conversion efficiency. For parametric amplification, a beta-barium borate crystal is pumped by a 140 W, 1 ps Yb:YAG InnoSlab amplifier at 3.25 MHz repetition rate. The broadband seed is generated via supercontinuum generation in a YAG crystal.

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Cited by 41 publications
(19 citation statements)
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“…A white-light continuum is difficult to achieve with long pump pulses [45], but is here successfully established using a 4 mm YAG crystal pumped with pulse energies of about 7 μJ, focused using an f = 80 mm lens. Similar to earlier results [46], the continuum smoothly covers the range 480-950 nm and makes an ideal seed light for the NOPA process in a 2 mm thick type-I BBO crystal at 37°. The pump pulses at 344 nm are derived from the thin-disk laser by frequency-tripling in a sequence of two group-velocity-compensating BBO crystals [44], a 0.8 mm thick type-I crystal at 23.5°for second harmonic generation followed by a 1.5 mm thick type-II crystal at 62.8°for sum-frequency mixing.…”
Section: Experimental Setup-tunable Visible Noncollinear Optical Parasupporting
confidence: 84%
“…A white-light continuum is difficult to achieve with long pump pulses [45], but is here successfully established using a 4 mm YAG crystal pumped with pulse energies of about 7 μJ, focused using an f = 80 mm lens. Similar to earlier results [46], the continuum smoothly covers the range 480-950 nm and makes an ideal seed light for the NOPA process in a 2 mm thick type-I BBO crystal at 37°. The pump pulses at 344 nm are derived from the thin-disk laser by frequency-tripling in a sequence of two group-velocity-compensating BBO crystals [44], a 0.8 mm thick type-I crystal at 23.5°for second harmonic generation followed by a 1.5 mm thick type-II crystal at 62.8°for sum-frequency mixing.…”
Section: Experimental Setup-tunable Visible Noncollinear Optical Parasupporting
confidence: 84%
“…Construction of wide-field three-photon instrumentation will become much easier with the development of commercially available OPCPA designs offering several tens of Watts of power throughout the visible and near-infrared spectrum4547. Excitation can therefore be performed faster, and over larger areas compared to the Ti:Sapphire-based system used here.…”
Section: Discussionmentioning
confidence: 99%
“…Indeed, the availability of picosecond pulse-generated SC with a well-behaved spectral phase that is compressible down to transform-limit paved new avenues in the development of picosecond-laser pumped noncollinear optical parametric amplifiers [213] and of a whole new generation of compact SC-seeded OPCPA systems. These systems are built around amplified solely sub-picosecond and picosecond lasers, such as Yb:KYW [214], Yb:YAG [51,207,[215][216][217] and Yb-fibre [218,219], and are designed to provide few optical cycle pulses in the near-and mid-infrared at very high repetition rates. Finally, picosecond SC serves as a seed signal in the mid-infrared optical parametric amplifiers driven by amplified picosecond Ho:YAG lasers [220,221].…”
Section: Laser Hostsmentioning
confidence: 99%